Optical image capturing system

ABSTRACT

An optical image capturing system includes, along the optical axis in order from an object side to an image side, a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, and a seventh lens. At least one lens among the first to the sixth lenses has positive refractive force. The seventh lens can have negative refractive force, wherein both surfaces thereof are aspheric, and at least one surface thereof has an inflection point. The lenses in the optical image capturing system which have refractive power include the first to the seventh lenses. The optical image capturing system can increase aperture value and improve the imagining quality for use in compact cameras.

BACKGROUND OF THE INVENTION

1. Technical Field

The present invention relates generally to an optical system, and moreparticularly to a compact optical image capturing system for anelectronic device.

2. Description of Related Art

In recent years, with the rise of portable electronic devices havingcamera functionalities, the demand for an optical image capturing systemis raised gradually. The image sensing device of the ordinaryphotographing camera is commonly selected from charge coupled device(CCD) or complementary metal-oxide semiconductor sensor (CMOS Sensor).In addition, as advanced semiconductor manufacturing technology enablesthe minimization of the pixel size of the image sensing device, thedevelopment of the optical image capturing system towards the field ofhigh pixels. Therefore, the requirement for high imaging quality israpidly raised.

The conventional optical system of the portable electronic deviceusually has five or six lenses. However, the optical system is asked totake pictures in a dark environment, in other words, the optical systemis asked to have a large aperture. The conventional optical systemprovides high optical performance as required.

It is an important issue to increase the quantity of light entering thelens. In addition, the modern lens is also asked to have severalcharacters, including high image quality.

BRIEF SUMMARY OF THE INVENTION

The aspect of embodiment of the present disclosure directs to an opticalimage capturing system and an optical image capturing lens which usecombination of refractive powers, convex and concave surfaces ofseven-piece optical lenses (the convex or concave surface in thedisclosure denotes the geometrical shape of an image-side surface or anobject-side surface of each lens on an optical axis) to increase thequantity of incoming light of the optical image capturing system, and toimprove imaging quality for image formation, so as to be applied tominimized electronic products.

The term and its definition to the lens parameter in the embodiment ofthe present are shown as below for further reference.

The lens parameter related to a length or a height in the lens:

A maximum height for image formation of the optical image capturingsystem is denoted by HOI. A height of the optical image capturing systemis denoted by HOS. A distance from the object-side surface of the firstlens to the image-side surface of the seventh lens is denoted by InTL. Adistance from the first lens to the second lens is denoted by IN12(instance). A central thickness of the first lens of the optical imagecapturing system on the optical axis is denoted by TP1 (instance).

The lens parameter related to a material in the lens:

An Abbe number of the first lens in the optical image capturing systemis denoted by NA1 (instance). A refractive index of the first lens isdenoted by Nd1 (instance).

The lens parameter related to a view angle in the lens:

A view angle is denoted by AF. Half of the view angle is denoted by HAF.A major light angle is denoted by MRA.

The lens parameter related to exit/entrance pupil in the lens:

An entrance pupil diameter of the optical image capturing system isdenoted by HEP. For any surface of any lens, a maximum effective halfdiameter (EHD) is a perpendicular distance between an optical axis and acrossing point on the surface where the incident light with a maximumviewing angle of the system passing the very edge of the entrance pupil.For example, the maximum effective half diameter of the object-sidesurface of the first lens is denoted by EHD11, the maximum effectivehalf diameter of the image-side surface of the first lens is denoted byEHD12, the maximum effective half diameter of the object-side surface ofthe second lens is denoted by EHD21, the maximum effective half diameterof the image-side surface of the second lens is denoted by EHD22, and soon.

The lens parameter related to an arc length of the shape of a surfaceand a surface profile:

For any surface of any lens, a profile curve length of the maximumeffective half diameter is, by definition, measured from a start pointwhere the optical axis of the belonging optical image capturing systempasses through the surface of the lens, along a surface profile of thelens, and finally to an end point of the maximum effective half diameterthereof. In other words, the curve length between the aforementionedstart and end points is the profile curve length of the maximumeffective half diameter, which is denoted by ARS. For example, theprofile curve length of the maximum effective half diameter of theobject-side surface of the first lens is denoted by ARS11, the profilecurve length of the maximum effective half diameter of the image-sidesurface of the first lens is denoted by ARS12, the profile curve lengthof the maximum effective half diameter of the object-side surface of thesecond lens is denoted by ARS21, the profile curve length of the maximumeffective half diameter of the image-side surface of the second lens isdenoted by ARS22, and so on.

For any surface of any lens, a profile curve length of a half of theentrance pupil diameter (HEP) is, by definition, measured from a startpoint where the optical axis of the belonging optical image capturingsystem passes through the surface of the lens, along a surface profileof the lens, and finally to a coordinate point of a perpendiculardistance where is a half of the entrance pupil diameter away from theoptical axis. In other words, the curve length between theaforementioned stat point and the coordinate point is the profile curvelength of a half of the entrance pupil diameter (HEP), and is denoted byARE. For example, the profile curve length of a half of the entrancepupil diameter (HEP) of the object-side surface of the first lens isdenoted by ARE11, the profile curve length of a half of the entrancepupil diameter (HEP) of the image-side surface of the first lens isdenoted by ARE12, the profile curve length of a half of the entrancepupil diameter (HEP) of the object-side surface of the second lens isdenoted by ARE21, the profile curve length of a half of the entrancepupil diameter (HEP) of the image-side surface of the second lens isdenoted by ARE22, and so on.

The lens parameter related to a depth of the lens shape:

A distance in parallel with the optical axis from a point where theoptical axis passes through to an end point of the maximum effectivesemi diameter on the object-side surface of the seventh lens is denotedby InRS71 (the depth of the maximum effective semi diameter). A distancein parallel with the optical axis from a point where the optical axispasses through to an end point of the maximum effective semi diameter onthe image-side surface of the seventh lens is denoted by InRS72 (thedepth of the maximum effective semi diameter). The depth of the maximumeffective semi diameter (sinkage) on the object-side surface or theimage-side surface of any other lens is denoted in the same manner.

The lens parameter related to the lens shape:

A critical point C is a tangent point on a surface of a specific lens,and the tangent point is tangent to a plane perpendicular to the opticalaxis and the tangent point cannot be a crossover point on the opticalaxis. Following the above description, a distance perpendicular to theoptical axis between a critical point C51 on the object-side surface ofthe fifth lens and the optical axis is HVT51 (instance), and a distanceperpendicular to the optical axis between a critical point C52 on theimage-side surface of the fifth lens and the optical axis is HVT52(instance). A distance perpendicular to the optical axis between acritical point C61 on the object-side surface of the sixth lens and theoptical axis is HVT61 (instance), and a distance perpendicular to theoptical axis between a critical point C62 on the image-side surface ofthe sixth lens and the optical axis is HVT62 (instance). A distanceperpendicular to the optical axis between a critical point on theobject-side or image-side surface of other lenses, such as the seventhlens, and the optical axis is denoted in the same manner.

The object-side surface of the seventh lens has one inflection pointIF711 which is nearest to the optical axis, and the sinkage value of theinflection point IF711 is denoted by SGI711 (instance). A distanceperpendicular to the optical axis between the inflection point IF711 andthe optical axis is HIF711 (instance). The image-side surface of theseventh lens has one inflection point IF721 which is nearest to theoptical axis, and the sinkage value of the inflection point IF721 isdenoted by SGI721 (instance). A distance perpendicular to the opticalaxis between the inflection point IF721 and the optical axis is HIF721(instance).

The object-side surface of the seventh lens has one inflection pointIF712 which is the second nearest to the optical axis, and the sinkagevalue of the inflection point IF712 is denoted by SGI712 (instance). Adistance perpendicular to the optical axis between the inflection pointIF712 and the optical axis is HIF712 (instance). The image-side surfaceof the seventh lens has one inflection point IF722 which is the secondnearest to the optical axis, and the sinkage value of the inflectionpoint IF722 is denoted by SGI722 (instance). A distance perpendicular tothe optical axis between the inflection point IF722 and the optical axisis HIF722 (instance).

The object-side surface of the seventh lens has one inflection pointIF713 which is the third nearest to the optical axis, and the sinkagevalue of the inflection point IF713 is denoted by SGI713 (instance). Adistance perpendicular to the optical axis between the inflection pointIF713 and the optical axis is HIF713 (instance). The image-side surfaceof the seventh lens has one inflection point IF723 which is the thirdnearest to the optical axis, and the sinkage value of the inflectionpoint IF723 is denoted by SGI723 (instance). A distance perpendicular tothe optical axis between the inflection point IF723 and the optical axisis HIF723 (instance).

The object-side surface of the seventh lens has one inflection pointIF714 which is the fourth nearest to the optical axis, and the sinkagevalue of the inflection point IF714 is denoted by SGI714 (instance). Adistance perpendicular to the optical axis between the inflection pointIF714 and the optical axis is HIF714 (instance). The image-side surfaceof the seventh lens has one inflection point IF724 which is the fourthnearest to the optical axis, and the sinkage value of the inflectionpoint IF724 is denoted by SGI724 (instance). A distance perpendicular tothe optical axis between the inflection point IF724 and the optical axisis HIF724 (instance).

An inflection point, a distance perpendicular to the optical axisbetween the inflection point and the optical axis, and a sinkage valuethereof on the object-side surface or image-side surface of other lensesis denoted in the same manner.

The lens parameter related to an aberration:

Optical distortion for image formation in the optical image capturingsystem is denoted by ODT. TV distortion for image formation in theoptical image capturing system is denoted by TDT. Further, the range ofthe aberration offset for the view of image formation may be limited to50%-100% field. An offset of the spherical aberration is denoted by DFS.An offset of the coma aberration is denoted by DFC.

Transverse aberration on an edge of an aperture is denoted by STA, whichstands for STOP transverse aberration, and is used to evaluate theperformance of one specific optical image capturing system. Thetransverse aberration of light in any field of view can be calculatedwith a tangential fan or a sagittal fan. More specifically, thetransverse aberration caused when the longest operation wavelength(e.g., 650 nm) and the shortest operation wavelength (e.g., 470 nm) passthrough the edge of the aperture can be used as the reference forevaluating performance. The coordinate directions of the aforementionedtangential fan can be further divided into a positive direction (upperlight) and a negative direction (lower light). The longest operationwavelength which passes through the edge of the aperture has an imagingposition on the image plane in a particular field of view, and thereference wavelength of the mail light (e.g., 555 nm) has anotherimaging position on the image plane in the same field of view. Thetransverse aberration caused when the longest operation wavelengthpasses through the edge of the aperture is defined as a distance betweenthese two imaging positions. Similarly, the shortest operationwavelength which passes through the edge of the aperture has an imagingposition on the image plane in a particular field of view, and thetransverse aberration caused when the shortest operation wavelengthpasses through the edge of the aperture is defined as a distance betweenthe imaging position of the shortest operation wavelength and theimaging position of the reference wavelength. The performance of theoptical image capturing system can be considered excellent if thetransverse aberrations of the shortest and the longest operationwavelength which pass through the edge of the aperture and image on theimage plane in 0.7 field of view (i.e., 0.7 times the height for imageformation HOI) are both less than 100 μm. Furthermore, for a stricterevaluation, the performance cannot be considered excellent unless thetransverse aberrations of the shortest and the longest operationwavelength which pass through the edge of the aperture and image on theimage plane in 0.7 field of view are both less than 80 μm.

The optical image capturing system has a maximum image height HOI on theimage plane vertical to the optical axis. A transverse aberration at 0.7HOI in the positive direction of the tangential fan after the longestoperation wavelength of visible light passing through the edge of theaperture is denoted by PLTA; a transverse aberration at 0.7 HOI in thepositive direction of the tangential fan after the shortest operationwavelength of visible light passing through the edge of the aperture isdenoted by PSTA; a transverse aberration at 0.7 HOI in the negativedirection of the tangential fan after the longest operation wavelengthof visible light passing through the edge of the aperture is denoted byNLTA; a transverse aberration at 0.7 HOI in the negative direction ofthe tangential fan after the shortest operation wavelength of visiblelight passing through the edge of the aperture is denoted by NSTA; atransverse aberration at 0.7 HOI of the sagittal fan after the longestoperation wavelength of visible light passing through the edge of theaperture is denoted by SLTA; a transverse aberration at 0.7 HOI of thesagittal fan after the shortest operation wavelength of visible lightpassing through the edge of the aperture is denoted by SSTA.

The present invention provides an optical image capturing system capableof focusing for both visible light and infrared light (i.e., dual mode)with certain performance, in which the seventh lens is provided with aninflection point at the object-side surface or at the image-side surfaceto adjust the incident angle of each view field and modify the ODT andthe TDT. In addition, the surfaces of the seventh lens are capable ofmodifying the optical path to improve the imagining quality.

The optical image capturing system of the present invention includes afirst lens, a second lens, a third lens, a fourth lens, a fifth lens, asixth lens, a seventh lens, and an image plane in order along an opticalaxis from an object side to an image side. At least one lens among thefirst to the seventh lens is made of glass. At least four lenses amongthe first to the seventh lens are made of plastic. The first lens hasrefractive power. The optical image capturing system satisfies:1.0≤f/HEP≤10.0; 0 deg≤HAF≤150 deg; and 0.9≤2(ARE/HEP)≤1.5;

where f1, f2, f3, f4, f5, f6, and f7 are respectively the focal lengthsof the first lens to the seventh lens; f is a focal length of theoptical image capturing system; HEP is an entrance pupil diameter of theoptical image capturing system; HOS is a distance in parallel with theoptical axis between an object-side surface, which face the object side,of the first lens and the image plane; InTL is a distance between theobject-side surface of the first lens and the image-side surface of theseventh lens on the optical axis; HAF is a half of the maximum fieldangle; ARE is a profile curve length measured from a start point wherethe optical axis of the belonging optical image capturing system passesthrough the surface of the lens, along a surface profile of the lens,and finally to a coordinate point of a perpendicular distance where is ahalf of the entrance pupil diameter away from the optical axis.

The present invention further provides an optical image capturingsystem, including a first lens, a second lens, a third lens, a fourthlens, a fifth lens, a sixth lens, a seventh lens, and an image plane inorder along an optical axis from an object side to an image side. Thefirst lens is made of glass, while at least five lenses among the secondlens to the seventh lens is made of plastic. The first lens hasrefractive power, and an object-side surface thereof near the opticalaxis could be convex. The second lens has refractive power. The thirdlens has refractive power. The fourth lens has refractive power. Thefifth lens has refractive power. The sixth lens has refractive power.The seventh lens has refractive power, wherein the object-side surfaceand the image-side surface thereof are both aspheric surfaces. At leastone lens among the second lens to the seventh lens has positiverefractive power. The optical image capturing system satisfies:1.0≤f/HEP≤10.0; 0<InTL/HOS<0.9; 0 deg<HAF≤150 deg; and0.9≤2(ARE/HEP)≤1.5;

where f1, f2, f3, f4, f5, f6, and f7 are respectively the focal lengthsof the first lens to the seventh lens; f is a focal length of theoptical image capturing system; HEP is an entrance pupil diameter of theoptical image capturing system; HOS is a distance in parallel with theoptical axis between an object-side surface, which face the object side,of the first lens and the image plane; InTL is a distance between theobject-side surface of the first lens and the image-side surface of theseventh lens on the optical axis; HAF is a half of the maximum fieldangle; ARE is a profile curve length measured from a start point wherethe optical axis of the belonging optical image capturing system passesthrough the surface of the lens, along a surface profile of the lens,and finally to a coordinate point of a perpendicular distance where is ahalf of the entrance pupil diameter away from the optical axis.

The present invention further provides an optical image capturingsystem, including a first lens, a second lens, a third lens, a fourthlens, a fifth lens, a sixth lens, a seventh lens, and an image plane, inorder along an optical axis from an object side to an image side. Thenumber of the lenses having refractive power in the optical imagecapturing system is seven. Five lenses among the first to the seventhlenses are made of plastic, while the other two lenses are made ofglass. The first lens has negative refractive power, and the second lenshas refractive power. The third lens has refractive power. The fourthlens has refractive power. The fifth lens has refractive power. Thesixth lens has refractive power. The seventh lens has refractive power.The optical image capturing system satisfies:1.0≤f/HEP≤6.0; 0<InTL/HOS<0.9; 0 deg<HAF≤150 deg; and0.9≤2(ARE/HEP)≤1.5;

where f1, f2, f3, f4, f5, f6, and f7 are respectively the focal lengthsof the first lens to the seventh lens; f is a focal length of theoptical image capturing system; HEP is an entrance pupil diameter of theoptical image capturing system; HOS is a distance in parallel with theoptical axis between an object-side surface, which face the object side,of the first lens and the image plane; InTL is a distance between theobject-side surface of the first lens and the image-side surface of theseventh lens on the optical axis; HAF is a half of the maximum fieldangle; ARE is a profile curve length measured from a start point wherethe optical axis of the belonging optical image capturing system passesthrough the surface of the lens, along a surface profile of the lens,and finally to a coordinate point of a perpendicular distance where is ahalf of the entrance pupil diameter away from the optical axis.

For any surface of any lens, the profile curve length within theeffective half diameter affects the ability of the surface to correctaberration and differences between optical paths of light in differentfields of view. With longer profile curve length, the ability to correctaberration is better. However, the difficulty of manufacturing increasesas well. Therefore, the profile curve length within the effective halfdiameter of any surface of any lens has to be controlled. The ratiobetween the profile curve length (ARS) within the effective halfdiameter of one surface and the thickness (TP) of the lens, which thesurface belonged to, on the optical axis (i.e., ARS/TP) has to beparticularly controlled. For example, the profile curve length of themaximum effective half diameter of the object-side surface of the firstlens is denoted by ARS11, the thickness of the first lens on the opticalaxis is TP1, and the ratio between these two parameters is ARS11/TP1;the profile curve length of the maximum effective half diameter of theimage-side surface of the first lens is denoted by ARS12, and the ratiobetween ARS12 and TP1 is ARS12/TP1. The profile curve length of themaximum effective half diameter of the object-side surface of the secondlens is denoted by ARS21, the thickness of the second lens on theoptical axis is TP2, and the ratio between these two parameters isARS21/TP2; the profile curve length of the maximum effective halfdiameter of the image-side surface of the second lens is denoted byARS22, and the ratio between ARS22 and TP2 is ARS22/TP2. For any surfaceof other lenses in the optical image capturing system, the ratio betweenthe profile curve length of the maximum effective half diameter thereofand the thickness of the lens which the surface belonged to is denotedin the same manner.

For any surface of any lens, the profile curve length within a half ofthe entrance pupil diameter (HEP) affects the ability of the surface tocorrect aberration and differences between optical paths of light indifferent fields of view. With longer profile curve length, the abilityto correct aberration is better. However, the difficulty ofmanufacturing increases as well. Therefore, the profile curve lengthwithin a half of the entrance pupil diameter (HEP) of any surface of anylens has to be controlled. The ratio between the profile curve length(ARE) within a half of the entrance pupil diameter (HEP) of one surfaceand the thickness (TP) of the lens, which the surface belonged to, onthe optical axis (i.e., ARE/TP) has to be particularly controlled. Forexample, the profile curve length of a half of the entrance pupildiameter (HEP) of the object-side surface of the first lens is denotedby ARE11, the thickness of the first lens on the optical axis is TP1,and the ratio between these two parameters is ARE11/TP1; the profilecurve length of a half of the entrance pupil diameter (HEP) of theimage-side surface of the first lens is denoted by ARE12, and the ratiobetween ARE12 and TP1 is ARE12/TP1. The profile curve length of a halfof the entrance pupil diameter (HEP) of the object-side surface of thesecond lens is denoted by ARE21, the thickness of the second lens on theoptical axis is TP2, and the ratio between these two parameters isARE21/TP2; the profile curve length of a half of the entrance pupildiameter (HEP) of the image-side surface of the second lens is denotedby ARE22, and the ratio between ARE22 and TP2 is ARE22/TP2. For anysurface of other lenses in the optical image capturing system, the ratiobetween the profile curve length of a half of the entrance pupildiameter (HEP) thereof and the thickness of the lens which the surfacebelonged to is denoted in the same manner.

In an embodiment, a height of the optical image capturing system (HOS)can be reduced if |f1|>|f7|.

In an embodiment, when |f2|+|f3|+|f4|+|f5|+|f6| and |f1|+|f7| of thelenses satisfy the aforementioned conditions, at least one lens amongthe second to the sixth lenses could have weak positive refractive poweror weak negative refractive power. Herein the weak refractive powermeans the absolute value of the focal length of one specific lens isgreater than 10. When at least one lens among the second to the sixthlenses has weak positive refractive power, it may share the positiverefractive power of the first lens, and on the contrary, when at leastone lens among the second to the sixth lenses has weak negativerefractive power, it may fine turn and correct the aberration of thesystem.

In an embodiment, the seventh lens could have negative refractive power,and an image-side surface thereof is concave, it may reduce back focallength and size. Besides, the seventh lens can have at least aninflection point on at least a surface thereof, which may reduce anincident angle of the light of an off-axis field of view and correct theaberration of the off-axis field of view.

BRIEF DESCRIPTION OF THE SEVERAL VIEWS OF THE DRAWINGS

The present invention will be best understood by referring to thefollowing detailed description of some illustrative embodiments inconjunction with the accompanying drawings, in which

FIG. 1A is a schematic diagram of a first embodiment of the presentinvention;

FIG. 1B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the first embodiment of thepresent application;

FIG. 1C shows a tangential fan and a sagittal fan of the optical imagecapturing system of the first embodiment of the present application, anda transverse aberration diagram at 0.7 field of view when a longestoperation wavelength and a shortest operation wavelength pass through anedge of an aperture;

FIG. 2A is a schematic diagram of a second embodiment of the presentinvention;

FIG. 2B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the second embodiment of thepresent application;

FIG. 2C shows a tangential fan and a sagittal fan of the optical imagecapturing system of the second embodiment of the present application,and a transverse aberration diagram at 0.7 field of view when a longestoperation wavelength and a shortest operation wavelength pass through anedge of an aperture;

FIG. 3A is a schematic diagram of a third embodiment of the presentinvention;

FIG. 3B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the third embodiment of thepresent application;

FIG. 3C shows a tangential fan and a sagittal fan of the optical imagecapturing system of the third embodiment of the present application, anda transverse aberration diagram at 0.7 field of view when a longestoperation wavelength and a shortest operation wavelength pass through anedge of an aperture;

FIG. 4A is a schematic diagram of a fourth embodiment of the presentinvention;

FIG. 4B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the fourth embodiment of thepresent application;

FIG. 4C shows a tangential fan and a sagittal fan of the optical imagecapturing system of the fourth embodiment of the present application,and a transverse aberration diagram at 0.7 field of view when a longestoperation wavelength and a shortest operation wavelength pass through anedge of an aperture;

FIG. 5A is a schematic diagram of a fifth embodiment of the presentinvention;

FIG. 5B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the fifth embodiment of thepresent application;

FIG. 5C shows a tangential fan and a sagittal fan of the optical imagecapturing system of the fifth embodiment of the present application, anda transverse aberration diagram at 0.7 field of view when a longestoperation wavelength and a shortest operation wavelength pass through anedge of an aperture;

FIG. 6A is a schematic diagram of a sixth embodiment of the presentinvention;

FIG. 6B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the sixth embodiment of thepresent application;

FIG. 6C shows a tangential fan and a sagittal fan of the optical imagecapturing system of the sixth embodiment of the present application, anda transverse aberration diagram at 0.7 field of view when a longestoperation wavelength and a shortest operation wavelength pass through anedge of an aperture;

FIG. 7A is a schematic diagram of a seventh embodiment of the presentinvention;

FIG. 7B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the seventh embodiment of thepresent application;

FIG. 7C shows a tangential fan and a sagittal fan of the optical imagecapturing system of the seventh embodiment of the present application,and a transverse aberration diagram at 0.7 field of view when a longestoperation wavelength and a shortest operation wavelength pass through anedge of an aperture;

FIG. 8A is a schematic diagram of a eighth embodiment of the presentinvention;

FIG. 8B shows curve diagrams of longitudinal spherical aberration,astigmatic field, and optical distortion of the optical image capturingsystem in the order from left to right of the eighth embodiment of thepresent application; and

FIG. 8C shows a tangential fan and a sagittal fan of the optical imagecapturing system of the eighth embodiment of the present application,and a transverse aberration diagram at 0.7 field of view when a longestoperation wavelength and a shortest operation wavelength pass through anedge of an aperture.

DETAILED DESCRIPTION OF THE INVENTION

An optical image capturing system of the present invention includes afirst lens, a second lens, a third lens, a fourth lens, a fifth lens, asixth lens, a seventh lens, and an image plane from an object side to animage side. The optical image capturing system further is provided withan image sensor at an image plane, wherein the image heights of thefollowing embodiments are all around 3.91 mm.

The optical image capturing system can work in three wavelengths,including 486.1 nm, 587.5 nm, and 656.2 nm, wherein 587.5 nm is the mainreference wavelength and is the reference wavelength for obtaining thetechnical characters. The optical image capturing system can also workin five wavelengths, including 470 nm, 510 nm, 555 nm, 610 nm, and 650nm wherein 555 nm is the main reference wavelength, and is the referencewavelength for obtaining the technical characters.

The optical image capturing system of the present invention satisfies0.5≤ΣPPR/|ΣNPR|≤15, and a preferable range is 1≤ΣPPR/|ΣNPR|≤3.0, wherePPR is a ratio of the focal length f of the optical image capturingsystem to a focal length fp of each of lenses with positive refractivepower; NPR is a ratio of the focal length f of the optical imagecapturing system to a focal length fn of each of lenses with negativerefractive power; ΣPPR is a sum of the PPRs of each positive lens; andΣNPR is a sum of the NPRs of each negative lens. It is helpful forcontrol of an entire refractive power and an entire length of theoptical image capturing system.

The image sensor is provided on the image plane. The optical imagecapturing system of the present invention satisfies HOS/HOI≤10; and0.5≤HOS/f≤10, and a preferable range is 1≤HOS/HOI≤5; and 1≤HOS/f≤7,where HOI is a half of a diagonal of an effective sensing area of theimage sensor, i.e., the maximum image height, and HOS is a height of theoptical image capturing system, i.e. a distance on the optical axisbetween the object-side surface of the first lens and the image plane.It is helpful for reduction of the size of the system for used incompact cameras.

The optical image capturing system of the present invention further isprovided with an aperture to increase image quality.

In the optical image capturing system of the present invention, theaperture could be a front aperture or a middle aperture, wherein thefront aperture is provided between the object and the first lens, andthe middle is provided between the first lens and the image plane. Thefront aperture provides a long distance between an exit pupil of thesystem and the image plane, which allows more elements to be installed.The middle could enlarge a view angle of view of the system and increasethe efficiency of the image sensor. The optical image capturing systemsatisfies 0.2≤InS/HOS≤1.1, where InS is a distance between the apertureand the image-side surface of the sixth lens. It is helpful for sizereduction and wide angle.

The optical image capturing system of the present invention satisfies0.1≤ΣTP/InTL≤0.9, where InTL is a distance between the object-sidesurface of the first lens and the image-side surface of the seventhlens, and ΣTP is a sum of central thicknesses of the lenses on theoptical axis. It is helpful for the contrast of image and yield rate ofmanufacture and provides a suitable back focal length for installationof other elements.

The optical image capturing system of the present invention satisfies0.001≤|R1/R2|≤20, and a preferable range is 0.01≤|R1/R2|<10, where R1 isa radius of curvature of the object-side surface of the first lens, andR2 is a radius of curvature of the image-side surface of the first lens.It provides the first lens with a suitable positive refractive power toreduce the increase rate of the spherical aberration.

The optical image capturing system of the present invention satisfies−7<(R13−R14)/(R13+R14)<50, where R13 is a radius of curvature of theobject-side surface of the seventh lens, and R14 is a radius ofcurvature of the image-side surface of the seventh lens. It may modifythe astigmatic field curvature.

The optical image capturing system of the present invention satisfiesIN12/f≤3.0, where IN12 is a distance on the optical axis between thefirst lens and the second lens. It may correct chromatic aberration andimprove the performance.

The optical image capturing system of the present invention satisfiesIN67/f≤0.8, where IN67 is a distance on the optical axis between thesixth lens and the seventh lens. It may correct chromatic aberration andimprove the performance.

The optical image capturing system of the present invention satisfies0.1≤(TP1+IN12)/TP2≤10, where TP1 is a central thickness of the firstlens on the optical axis, and TP2 is a central thickness of the secondlens on the optical axis. It may control the sensitivity of manufactureof the system and improve the performance.

The optical image capturing system of the present invention satisfies0.1≤(TP7+IN67)/TP6≤10, where TP6 is a central thickness of the sixthlens on the optical axis, TP7 is a central thickness of the seventh lenson the optical axis, and IN67 is a distance between the sixth lens andthe seventh lens. It may control the sensitivity of manufacture of thesystem and improve the performance.

The optical image capturing system of the present invention satisfies0.1≤TP4/(IN34+TP4+IN45)<1, where TP3 is a central thickness of the thirdlens on the optical axis, TP4 is a central thickness of the fourth lenson the optical axis, TP5 is a central thickness of the fifth lens on theoptical axis, IN34 is a distance on the optical axis between the thirdlens and the fourth lens, IN45 is a distance on the optical axis betweenthe fourth lens and the fifth lens, and InTL is a distance between theobject-side surface of the first lens and the image-side surface of theseventh lens. It may fine tune and correct the aberration of theincident rays layer by layer, and reduce the height of the system.

The optical image capturing system satisfies 0 mm≤HVT71≤3 mm; 0mm<HVT72≤6 mm; 0≤HVT71/HVT72; 0 mm≤|SGC71|≤0.5 mm; 0 mm<|SGC72|≤2 mm;and 0<|SGC72|/(|SGC72|+TP7)≤0.9, where HVT71 a distance perpendicular tothe optical axis between the critical point C71 on the object-sidesurface of the seventh lens and the optical axis; HVT72 a distanceperpendicular to the optical axis between the critical point C72 on theimage-side surface of the seventh lens and the optical axis; SGC71 is adistance in parallel with the optical axis between an point on theobject-side surface of the seventh lens where the optical axis passesthrough and the critical point C71; SGC72 is a distance in parallel withthe optical axis between an point on the image-side surface of theseventh lens where the optical axis passes through and the criticalpoint C72. It is helpful to correct the off-axis view field aberration.

The optical image capturing system satisfies 0.2≤HVT72/HOI≤0.9, andpreferably satisfies 0.3≤HVT72/HOI≤0.8. It may help to correct theperipheral aberration.

The optical image capturing system satisfies 0≤HVT72/HOS≤0.5, andpreferably satisfies 0.2≤HVT72/HOS≤0.45. It may help to correct theperipheral aberration.

The optical image capturing system of the present invention satisfies0<SGI711/(SGI711+TP7)≤0.9; 0<SGI721/(SGI721+TP7)≤0.9, and it ispreferable to satisfy 0.1≤SGI711/(SGI711+TP7)≤0.6;0.1≤SGI721/(SGI721+TP7)≤0.6, where SGI711 is a displacement in parallelwith the optical axis, from a point on the object-side surface of theseventh lens, through which the optical axis passes, to the inflectionpoint on the object-side surface, which is the closest to the opticalaxis, and SGI721 is a displacement in parallel with the optical axis,from a point on the image-side surface of the seventh lens, throughwhich the optical axis passes, to the inflection point on the image-sidesurface, which is the closest to the optical axis.

The optical image capturing system of the present invention satisfies0<SGI712/(SGI712+TP7)≤0.9; 0<SGI722/(SGI722+TP7)≤0.9, and it ispreferable to satisfy 0.1≤SGI712/(SGI712+TP7)≤0.6;0.1≤SGI722/(SGI722+TP7)≤0.6, where SGI712 is a displacement in parallelwith the optical axis, from a point on the object-side surface of theseventh lens, through which the optical axis passes, to the inflectionpoint on the object-side surface, which is the second closest to theoptical axis, and SGI722 is a displacement in parallel with the opticalaxis, from a point on the image-side surface of the seventh lens,through which the optical axis passes, to the inflection point on theimage-side surface, which is the second closest to the optical axis.

The optical image capturing system of the present invention satisfies0.001 mm≤|HIF711|≤5 mm; 0.001 mm≤|HIF721|≤5 mm, and it is preferable tosatisfy 0.1 mm≤|HIF711|≤3.5 mm; 1.5 mm≤|HIF721|≤3.5 mm, where HIF711 isa distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the seventh lens, which is theclosest to the optical axis, and the optical axis; HIF721 is a distanceperpendicular to the optical axis between the inflection point on theimage-side surface of the seventh lens, which is the closest to theoptical axis, and the optical axis.

The optical image capturing system of the present invention satisfies0.001 mm≤|HIF712|≤5 mm; 0.001 mm≤|HIF722|≤5 mm, and it is preferable tosatisfy 0.1 mm≤|HIF722|≤3.5 mm; 0.1 mm≤|HIF712|≤3.5 mm, where HIF712 isa distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the seventh lens, which is thesecond closest to the optical axis, and the optical axis; HIF722 is adistance perpendicular to the optical axis between the inflection pointon the image-side surface of the seventh lens, which is the secondclosest to the optical axis, and the optical axis.

The optical image capturing system of the present invention satisfies0.001 mm≤|HIF713|≤5 mm; 0.001 mm≤|HIF723|≤5 mm, and it is preferable tosatisfy 0.1 mm≤|HIF723|≤3.5 mm; 0.1 mm≤|HIF713|S3.5 mm, where HIF713 isa distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the seventh lens, which is the thirdclosest to the optical axis, and the optical axis; HIF723 is a distanceperpendicular to the optical axis between the inflection point on theimage-side surface of the seventh lens, which is the third closest tothe optical axis, and the optical axis.

The optical image capturing system of the present invention satisfies0.001 mm≤|HIF714|≤5 mm; 0.001 mm≤|HIF724|≤5 mm, and it is preferable tosatisfy 0.1 mm≤|HIF724|≤3.5 mm; 0.1 mm≤|HIF714|≤3.5 mm, where HIF714 isa distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the seventh lens, which is thefourth closest to the optical axis, and the optical axis; HIF724 is adistance perpendicular to the optical axis between the inflection pointon the image-side surface of the seventh lens, which is the fourthclosest to the optical axis, and the optical axis.

In an embodiment, the lenses of high Abbe number and the lenses of lowAbbe number are arranged in an interlaced arrangement that could behelpful for correction of aberration of the system.

An equation of aspheric surface isz=ch ²/[1+[1(k+1)c ² h ²]^(0.5)]+A4h ⁴ +A6h ⁶ +A8h ⁸ +A10h ¹⁰ +A12h ¹²+A14h ¹⁴ +A16h ¹⁶ +A18h ¹⁸ +A20h ²⁰+  (1)

where z is a depression of the aspheric surface; k is conic constant; cis reciprocal of the radius of curvature; and A4, A6, A8, A10, A12, A14,A16, A18, and A20 are high-order aspheric coefficients.

In the optical image capturing system, the lenses could be made ofplastic or glass. The plastic lenses may reduce the weight and lower thecost of the system, and the glass lenses may control the thermal effectand enlarge the space for arrangement of the refractive power of thesystem. In addition, the opposite surfaces (object-side surface andimage-side surface) of the first to the seventh lenses could be asphericthat can obtain more control parameters to reduce aberration. The numberof aspheric glass lenses could be less than the conventional sphericalglass lenses, which is helpful for reduction of the height of thesystem.

When the lens has a convex surface, which means that the surface isconvex around a position, through which the optical axis passes, andwhen the lens has a concave surface, which means that the surface isconcave around a position, through which the optical axis passes.

The optical image capturing system of the present invention could beapplied in a dynamic focusing optical system. It is superior in thecorrection of aberration and high imaging quality so that it could beallied in lots of fields.

The optical image capturing system of the present invention couldfurther include a driving module to meet different demands, wherein thedriving module can be coupled with the lenses to move the lenses. Thedriving module can be a voice coil motor (VCM), which is used to movethe lens for focusing, or can be an optical image stabilization (OIS)component, which is used to lower the possibility of having the problemof image blurring which is caused by subtle movements of the lens whileshooting.

To meet different requirements, at least one lens among the first lensto the seventh lens of the optical image capturing system of the presentinvention can be a light filter, which filters out light of wavelengthshorter than 500 nm. Such effect can be achieved by coating on at leastone surface of the lens, or by using materials capable of filtering outshort waves to make the lens.

To meet different requirements, the image plane of the optical imagecapturing system in the present invention can be either flat or curved.If the image plane is curved (e.g., a sphere with a radius ofcurvature), the incidence angle required for focusing light on the imageplane can be decreased, which is not only helpful to shorten the lengthof the system (TTL), but also helpful to increase the relativeilluminance.

We provide several embodiments in conjunction with the accompanyingdrawings for the best understanding, which are:

First Embodiment

As shown in FIG. 1A and FIG. 1B, an optical image capturing system 10 ofthe first embodiment of the present invention includes, along an opticalaxis from an object side to an image side, a first lens 110, an aperture100, a second lens 120, a third lens 130, a fourth lens 140, a fifthlens 150, a sixth lens 160, a seventh lens 170, an infrared rays filter180, an image plane 190, and an image sensor 192. FIG. 1C shows atangential fan and a sagittal fan of the optical image capturing system10 of the first embodiment of the present application, and a transverseaberration diagram at 0.7 field of view when a longest operationwavelength and a shortest operation wavelength pass through an edge ofthe aperture 100.

The first lens 110 has negative refractive power and is made of plastic.An object-side surface 112 thereof, which faces the object side, is aconcave aspheric surface, and an image-side surface 114 thereof, whichfaces the image side, is a concave aspheric surface. The object-sidesurface 112 has an inflection point, and the image-side surface 114 hastwo inflection points. A profile curve length of the maximum effectivehalf diameter of an object-side surface of the first lens 110 is denotedby ARS11, and a profile curve length of the maximum effective halfdiameter of the image-side surface of the first lens 110 is denoted byARS12. A profile curve length of a half of an entrance pupil diameter(HEP) of the object-side surface of the first lens 110 is denoted byARE11, and a profile curve length of a half of the entrance pupildiameter (HEP) of the image-side surface of the first lens 110 isdenoted by ARE12. A thickness of the first lens 110 on the optical axisis TP1.

The first lens 110 satisfies SGI111=−0.1110 mm; SGI121=2.7120 mm;TP1=2.2761 mm; |SGI111|/(|SGI111|+TP1)=0.0465;|SGI121|/(|SGI121|+TP1)=0.5437, where a displacement in parallel withthe optical axis from a point on the object-side surface of the firstlens, through which the optical axis passes, to the inflection point onthe image-side surface, which is the closest to the optical axis isdenoted by SGI111, and a displacement in parallel with the optical axisfrom a point on the image-side surface of the first lens, through whichthe optical axis passes, to the inflection point on the image-sidesurface, which is the closest to the optical axis is denoted by SGI121.

The first lens 110 satisfies SGI112=0 mm; SGI122=4.2315 mm;|SGI112|/(|SGI112|+TP1)=0; |SGI122|/(|SGI122|+TP1)=0.6502, where adisplacement in parallel with the optical axis from a point on theobject-side surface of the first lens, through which the optical axispasses, to the inflection point on the image-side surface, which is thesecond closest to the optical axis is denoted by SGI112, and adisplacement in parallel with the optical axis from a point on theimage-side surface of the first lens, through which the optical axispasses, to the inflection point on the image-side surface, which is thesecond closest to the optical axis is denoted by SGI122.

The first lens 110 satisfies HIF111=12.8432 mm; HIF111/HOI=1.7127;HIF121=7.1744 mm; HIF121/HOI=0.9567, where a displacement perpendicularto the optical axis from a point on the object-side surface of the firstlens, through which the optical axis passes, to the inflection point,which is the closest to the optical axis is denoted by HIF111, and adisplacement perpendicular to the optical axis from a point on theimage-side surface of the first lens, through which the optical axispasses, to the inflection point, which is the closest to the opticalaxis is denoted by HIF121.

The first lens 110 satisfies HIF112=0 mm; HIF112/HOI=0; HIF122=9.8592mm; HIF122/HOI=1.3147, where a displacement perpendicular to the opticalaxis from a point on the object-side surface of the first lens, throughwhich the optical axis passes, to the inflection point, which is thesecond closest to the optical axis is denoted by HIF112, and adisplacement perpendicular to the optical axis from a point on theimage-side surface of the first lens, through which the optical axispasses, to the inflection point, which is the second closest to theoptical axis is denoted by HIF122.

The second lens 120 has positive refractive power and is made ofplastic. An object-side surface 122 thereof, which faces the objectside, is a convex aspheric surface, and an image-side surface 124thereof, which faces the image side, is a concave aspheric surface. Aprofile curve length of the maximum effective half diameter of anobject-side surface of the second lens 120 is denoted by ARS21, and aprofile curve length of the maximum effective half diameter of theimage-side surface of the second lens 120 is denoted by ARS22. A profilecurve length of a half of an entrance pupil diameter (HEP) of theobject-side surface of the second lens 120 is denoted by ARE21, and aprofile curve length of a half of the entrance pupil diameter (HEP) ofthe image-side surface of the second lens 120 is denoted by ARE22. Athickness of the second lens 120 on the optical axis is TP2.

For the second lens 120, a displacement in parallel with the opticalaxis from a point on the object-side surface of the second lens, throughwhich the optical axis passes, to the inflection point on the image-sidesurface, which is the closest to the optical axis is denoted by SGI211,and a displacement in parallel with the optical axis from a point on theimage-side surface of the second lens, through which the optical axispasses, to the inflection point on the image-side surface, which is theclosest to the optical axis is denoted by SGI221.

For the second lens, a displacement perpendicular to the optical axisfrom a point on the object-side surface of the second lens, throughwhich the optical axis passes, to the inflection point, which is theclosest to the optical axis is denoted by HIF211, and a displacementperpendicular to the optical axis from a point on the image-side surfaceof the second lens, through which the optical axis passes, to theinflection point, which is the closest to the optical axis is denoted byHIF221.

The third lens 130 has negative refractive power and is made of plastic.An object-side surface 132, which faces the object side, is a convexaspheric surface, and an image-side surface 134, which faces the imageside, is a concave aspheric surface. A profile curve length of themaximum effective half diameter of an object-side surface of the thirdlens 130 is denoted by ARS31, and a profile curve length of the maximumeffective half diameter of the image-side surface of the third lens 130is denoted by ARS32. A profile curve length of a half of an entrancepupil diameter (HEP) of the object-side surface of the third lens 130 isdenoted by ARE31, and a profile curve length of a half of the entrancepupil diameter (HEP) of the image-side surface of the third lens 130 isdenoted by ARE32. A thickness of the third lens 130 on the optical axisis TP3.

For the third lens 130, SGI311 is a displacement in parallel with theoptical axis, from a point on the object-side surface of the third lens,through which the optical axis passes, to the inflection point on theobject-side surface, which is the closest to the optical axis, andSGI321 is a displacement in parallel with the optical axis, from a pointon the image-side surface of the third lens, through which the opticalaxis passes, to the inflection point on the image-side surface, which isthe closest to the optical axis.

For the third lens 130, SGI312 is a displacement in parallel with theoptical axis, from a point on the object-side surface of the third lens,through which the optical axis passes, to the inflection point on theobject-side surface, which is the second closest to the optical axis,and SGI322 is a displacement in parallel with the optical axis, from apoint on the image-side surface of the third lens, through which theoptical axis passes, to the inflection point on the object-side surface,which is the second closest to the optical axis.

For the third lens 130, HIF311 is a distance perpendicular to theoptical axis between the inflection point on the object-side surface ofthe third lens, which is the closest to the optical axis, and theoptical axis; HIF321 is a distance perpendicular to the optical axisbetween the inflection point on the image-side surface of the thirdlens, which is the closest to the optical axis, and the optical axis.

For the third lens 130, HIF312 is a distance perpendicular to theoptical axis between the inflection point on the object-side surface ofthe third lens, which is the second closest to the optical axis, and theoptical axis; HIF322 is a distance perpendicular to the optical axisbetween the inflection point on the image-side surface of the thirdlens, which is the second closest to the optical axis, and the opticalaxis.

The fourth lens 140 has positive refractive power and is made ofplastic. An object-side surface 142, which faces the object side, is aconvex aspheric surface, and an image-side surface 144, which faces theimage side, is a convex aspheric surface. The object-side surface 142has an inflection point. A profile curve length of the maximum effectivehalf diameter of an object-side surface of the fourth lens 140 isdenoted by ARS41, and a profile curve length of the maximum effectivehalf diameter of the image-side surface of the fourth lens 140 isdenoted by ARS42. A profile curve length of a half of an entrance pupildiameter (HEP) of the object-side surface of the fourth lens 140 isdenoted by ARE41, and a profile curve length of a half of the entrancepupil diameter (HEP) of the image-side surface of the fourth lens 140 isdenoted by ARE42. A thickness of the fourth lens 140 on the optical axisis TP4.

The fourth lens 140 satisfies SGI411=0.0018 mm;|SGI411|/(|SGI411|+TP4)=0.0009, where SGI411 is a displacement inparallel with the optical axis, from a point on the object-side surfaceof the fourth lens, through which the optical axis passes, to theinflection point on the object-side surface, which is the closest to theoptical axis, and SGI421 is a displacement in parallel with the opticalaxis, from a point on the image-side surface of the fourth lens, throughwhich the optical axis passes, to the inflection point on the image-sidesurface, which is the closest to the optical axis.

For the fourth lens 140, SGI412 is a displacement in parallel with theoptical axis, from a point on the object-side surface of the fourthlens, through which the optical axis passes, to the inflection point onthe object-side surface, which is the second closest to the opticalaxis, and SGI422 is a displacement in parallel with the optical axis,from a point on the image-side surface of the fourth lens, through whichthe optical axis passes, to the inflection point on the object-sidesurface, which is the second closest to the optical axis.

The fourth lens 140 further satisfies HIF411=0.7191 mm;HIF411/HOI=0.0959, where HIF411 is a distance perpendicular to theoptical axis between the inflection point on the object-side surface ofthe fourth lens, which is the closest to the optical axis, and theoptical axis; HIF421 is a distance perpendicular to the optical axisbetween the inflection point on the image-side surface of the fourthlens, which is the closest to the optical axis, and the optical axis.

For the fourth lens 140, HIF412 is a distance perpendicular to theoptical axis between the inflection point on the object-side surface ofthe fourth lens, which is the second closest to the optical axis, andthe optical axis; HIF422 is a distance perpendicular to the optical axisbetween the inflection point on the image-side surface of the fourthlens, which is the second closest to the optical axis, and the opticalaxis.

The fifth lens 150 has positive refractive power and is made of plastic.An object-side surface 152, which faces the object side, is a concaveaspheric surface, and an image-side surface 154, which faces the imageside, is a convex aspheric surface. The object-side surface 152 and theimage-side surface 154 both have an inflection point. A profile curvelength of the maximum effective half diameter of an object-side surfaceof the fifth lens 150 is denoted by ARS51, and a profile curve length ofthe maximum effective half diameter of the image-side surface of thefifth lens 150 is denoted by ARS52. A profile curve length of a half ofan entrance pupil diameter (HEP) of the object-side surface of the fifthlens 150 is denoted by ARE51, and a profile curve length of a half ofthe entrance pupil diameter (HEP) of the image-side surface of the fifthlens 150 is denoted by ARE52. A thickness of the fifth lens 150 on theoptical axis is TP5.

The fifth lens 150 satisfies SGI511=−0.1246 mm; SGI521=−2.1477 mm;|SGI511|/(|SGI511|+TP5)=0.0284; |SGI521|/(|SGI521|+TP5)=0.3346, whereSGI511 is a displacement in parallel with the optical axis, from a pointon the object-side surface of the fifth lens, through which the opticalaxis passes, to the inflection point on the object-side surface, whichis the closest to the optical axis, and SGI521 is a displacement inparallel with the optical axis, from a point on the image-side surfaceof the fifth lens, through which the optical axis passes, to theinflection point on the image-side surface, which is the closest to theoptical axis.

For the fifth lens 150, SGI512 is a displacement in parallel with theoptical axis, from a point on the object-side surface of the fifth lens,through which the optical axis passes, to the inflection point on theobject-side surface, which is the second closest to the optical axis,and SGI522 is a displacement in parallel with the optical axis, from apoint on the image-side surface of the fifth lens, through which theoptical axis passes, to the inflection point on the object-side surface,which is the second closest to the optical axis.

The fifth lens 150 further satisfies HIF511=3.8179 mm; HIF521=4.5480 mm;HIF511/HOI=0.5091; HIF521/HOI=0.6065, where HIF511 is a distanceperpendicular to the optical axis between the inflection point on theobject-side surface of the fifth lens, which is the closest to theoptical axis, and the optical axis; HIF521 is a distance perpendicularto the optical axis between the inflection point on the image-sidesurface of the fifth lens, which is the closest to the optical axis, andthe optical axis.

For the fifth lens 150, HIF512 is a distance perpendicular to theoptical axis between the inflection point on the object-side surface ofthe fifth lens, which is the second closest to the optical axis, and theoptical axis; HIF522 is a distance perpendicular to the optical axisbetween the inflection point on the image-side surface of the fifthlens, which is the second closest to the optical axis, and the opticalaxis.

The sixth lens 160 has negative refractive power and is made of plastic.An object-side surface 162, which faces the object side, is a convexsurface, and an image-side surface 164, which faces the image side, is aconcave surface. The object-side surface 162 and the image-side surface164 both have an inflection point. Whereby, incident angle of each fieldof view for the sixth lens can be effectively adjusted to improveaberration. A profile curve length of the maximum effective halfdiameter of an object-side surface of the sixth lens 160 is denoted byARS61, and a profile curve length of the maximum effective half diameterof the image-side surface of the sixth lens 160 is denoted by ARS62. Aprofile curve length of a half of an entrance pupil diameter (HEP) ofthe object-side surface of the sixth lens 160 is denoted by ARE61, and aprofile curve length of a half of the entrance pupil diameter (HEP) ofthe image-side surface of the sixth lens 160 is denoted by ARE62. Athickness of the sixth lens 160 on the optical axis is TP6.

The sixth lens 160 satisfies SGI611=0.3208 mm; SGI621=0.5937 mm;|SGI611|/(|SGI611|+TP6)=0.5167; |SGI621|/(|SGI621|+TP6)=0.6643, whereSGI611 is a displacement in parallel with the optical axis, from a pointon the object-side surface of the sixth lens, through which the opticalaxis passes, to the inflection point on the object-side surface, whichis the closest to the optical axis, and SGI621 is a displacement inparallel with the optical axis, from a point on the image-side surfaceof the sixth lens, through which the optical axis passes, to theinflection point on the image-side surface, which is the closest to theoptical axis.

The sixth lens 160 further satisfies HIF611=1.9655 mm; HIF621=2.0041 mm;HIF611/HOI=0.2621; HIF621/HOI=0.2672, where HIF611 is a distanceperpendicular to the optical axis between the inflection point on theobject-side surface of the sixth lens, which is the closest to theoptical axis, and the optical axis; HIF621 is a distance perpendicularto the optical axis between the inflection point on the image-sidesurface of the sixth lens, which is the closest to the optical axis, andthe optical axis.

The seventh lens 170 has positive refractive power and is made ofplastic. An object-side surface 172, which faces the object side, is aconvex surface, and an image-side surface 174, which faces the imageside, is a concave surface. Whereby, it is helpful to shorten the focallength behind the seventh lens for miniaturization. The object-sidesurface 172 and the image-side surface 174 both have an inflectionpoint. A profile curve length of the maximum effective half diameter ofan object-side surface of the seventh lens 170 is denoted by ARS71, anda profile curve length of the maximum effective half diameter of theimage-side surface of the seventh lens 170 is denoted by ARS72. Aprofile curve length of a half of an entrance pupil diameter (HEP) ofthe object-side surface of the seventh lens 170 is denoted by ARE71, anda profile curve length of a half of the entrance pupil diameter (HEP) ofthe image-side surface of the seventh lens 170 is denoted by ARE72. Athickness of the seventh lens 170 on the optical axis is TP7.

The seventh lens 170 satisfies SGI711=0.5212 mm; SGI721=0.5668 mm;|SGI711|/(|SGI711|+TP7)=0.3179; |SGI721|/(|SGI721|+TP7)=0.3364, whereSGI711 is a displacement in parallel with the optical axis, from a pointon the object-side surface of the seventh lens, through which theoptical axis passes, to the inflection point on the object-side surface,which is the closest to the optical axis, and SGI721 is a displacementin parallel with the optical axis, from a point on the image-sidesurface of the seventh lens, through which the optical axis passes, tothe inflection point on the image-side surface, which is the closest tothe optical axis.

The seventh lens 170 further satisfies HIF711=1.6707 mm; HIF721=1.8616mm; HIF711/HOI=0.2228; HIF721/HOI=0.2482, where HIF711 is a distanceperpendicular to the optical axis between the inflection point on theobject-side surface of the seventh lens, which is the closest to theoptical axis, and the optical axis; HIF721 is a distance perpendicularto the optical axis between the inflection point on the image-sidesurface of the seventh lens, which is the closest to the optical axis,and the optical axis.

The features related to the inflection points in the present embodimentdescribed below are obtained with the main reference wavelength 555 nm.

The infrared rays filter 180 is made of glass and between the seventhlens 170 and the image plane 190. The infrared rays filter 180 gives nocontribution to the focal length of the system.

The optical image capturing system 10 of the first embodiment has thefollowing parameters, which are f=4.3019 mm; f/HEP=1.2; HAF=59.9968; andtan(HAF)=1.7318, where f is a focal length of the system; HAF is a halfof the maximum field angle; and HEP is an entrance pupil diameter.

The parameters of the lenses of the first embodiment are f1=−14.5286 mm;|f/f1|=0.2961; f7=8.2933; |f1|>f7; and |f1/f7|=1.7519, where f1 is afocal length of the first lens 110; and f7 is a focal length of theseventh lens 170.

The first embodiment further satisfies|f2|+|f3|+|f4|+|f5|+|f6|=144.7494; |f1|+|f7|=22.8219 and|f2|+|f3|+|f4|+|f5|+|f6|>|f1|+|f7|, where f2 is a focal length of thesecond lens 120, f3 is a focal length of the third lens 130, f4 is afocal length of the fourth lens 140, f5 is a focal length of the fifthlens 150, f6 is a focal length of the sixth lens 160, and f7 is a focallength of the seventh lens 170.

The optical image capturing system 10 of the first embodiment furthersatisfies ΣPPR=f/f2+f/f4+f/f5+f/f7=1.7384; ΣNPR=f/f1+f/f3+f/f6=−0.9999;ΣPPR/|ΣNPR|=1.7386; |f/f2|=0.1774; |f/f3|=0.0443; |f/f4|=0.4411;|f/f5|=0.6012; |f/f6|=0.6595; |f/f7|=0.5187, where PPR is a ratio of afocal length f of the optical image capturing system to a focal lengthfp of each of the lenses with positive refractive power; and NPR is aratio of a focal length f of the optical image capturing system to afocal length fn of each of lenses with negative refractive power.

The optical image capturing system 10 of the first embodiment furthersatisfies InTL+BFL=HOS; HOS=26.9789 mm; HOI=7.5 mm; HOS/HOI=3.5977;HOS/f=6.2715; InS=12.4615 mm; and InS/HOS=0.4619, where InTL is adistance between the object-side surface 112 of the first lens 110 andthe image-side surface 174 of the seventh lens 170; HOS is a height ofthe image capturing system, i.e. a distance between the object-sidesurface 112 of the first lens 110 and the image plane 190; InS is adistance between the aperture 100 and the image plane 190; HOI is a halfof a diagonal of an effective sensing area of the image sensor 192,i.e., the maximum image height; and BFL is a distance between theimage-side surface 174 of the seventh lens 170 and the image plane 190.

The optical image capturing system 10 of the first embodiment furthersatisfies ΣTP=16.0446 mm; and ΣTP/InTL=0.6559, where ΣTP is a sum of thethicknesses of the lenses 110-170 with refractive power. It is helpfulfor the contrast of image and yield rate of manufacture and provides asuitable back focal length for installation of other elements.

The optical image capturing system 10 of the first embodiment furthersatisfies |R1/R2|=129.9952, where R1 is a radius of curvature of theobject-side surface 112 of the first lens 110, and R2 is a radius ofcurvature of the image-side surface 114 of the first lens 110. Itprovides the first lens with a suitable positive refractive power toreduce the increase rate of the spherical aberration.

The optical image capturing system 10 of the first embodiment furthersatisfies (R13−R14)/(R13+R14)=−0.0806, where R13 is a radius ofcurvature of the object-side surface 172 of the seventh lens 170, andR14 is a radius of curvature of the image-side surface 174 of theseventh lens 170. It may modify the astigmatic field curvature.

The optical image capturing system 10 of the first embodiment furthersatisfies ΣPP=f2+f4+f5+f7=49.4535 mm; and f4/(f2+f4+f5+f7)=0.1972, whereΣPP is a sum of the focal lengths fp of each lens with positiverefractive power. It is helpful to share the positive refractive powerof the fourth lens 140 to other positive lenses to avoid the significantaberration caused by the incident rays.

The optical image capturing system 10 of the first embodiment furthersatisfies ΣNP=f1+f3+f6=−118.1178 mm; and f1/(f1+f3+f6)=0.1677, where ΣNPis a sum of the focal lengths fn of each lens with negative refractivepower. It is helpful to share the negative refractive power of the firstlens 110 to other negative lenses, which avoids the significantaberration caused by the incident rays.

The optical image capturing system 10 of the first embodiment furthersatisfies IN12=4.5524 mm; IN12/f=1.0582, where IN12 is a distance on theoptical axis between the first lens 110 and the second lens 120. It maycorrect chromatic aberration and improve the performance.

The optical image capturing system 10 of the first embodiment furthersatisfies TP1=2.2761 mm; TP2=0.2398 mm; and (TP1+IN12)/TP2=1.3032, whereTP1 is a central thickness of the first lens 110 on the optical axis,and TP2 is a central thickness of the second lens 120 on the opticalaxis. It may control the sensitivity of manufacture of the system andimprove the performance.

The optical image capturing system 10 of the first embodiment furthersatisfies TP6=0.3000 mm; TP7=1.1182 mm; and (TP7+IN67)/TP6=4.4322, whereTP6 is a central thickness of the sixth lens 160 on the optical axis,TP7 is a central thickness of the seventh lens 170 on the optical axis,and IN67 is a distance on the optical axis between the sixth lens 160and the seventh lens 170. It may control the sensitivity of manufactureof the system and lower the total height of the system.

The optical image capturing system 10 of the first embodiment furthersatisfies TP3=0.8369 mm; TP4=2.0022 mm; TP5=4.2706 mm; IN34=1.9268 mm;IN45=1.5153 mm; and TP4/(IN34+TP4+IN45)=0.3678, where TP3 is a centralthickness of the third lens 130 on the optical axis, TP4 is a centralthickness of the fourth lens 140 on the optical axis, TP5 is a centralthickness of the fifth lens 150 on the optical axis, IN34 is a distanceon the optical axis between the third lens 130 and the fourth lens 140,and IN45 is a distance on the optical axis between the fourth lens 140and the fifth lens 150. It may control the sensitivity of manufacture ofthe system and lower the total height of the system.

The optical image capturing system 10 of the first embodiment furthersatisfies InRS61=−0.7823 mm; InRS62=−0.2166 mm; and ∥nRS62|/TP6=0.722,where InRS61 is a displacement in parallel with the optical axis from apoint on the object-side surface 162 of the sixth lens 160, throughwhich the optical axis passes, to a point at the maximum effective semidiameter of the object-side surface 162 of the sixth lens; InRS62 is adisplacement in parallel with the optical axis from a point on theimage-side surface 164 of the sixth lens 160, through which the opticalaxis passes, to a point at the maximum effective semi diameter of theimage-side surface 164 of the sixth lens 160; and TP6 is a centralthickness of the sixth lens 160 on the optical axis. It is helpful formanufacturing and shaping of the lenses and is helpful to reduce thesize.

The optical image capturing system 10 of the first embodiment furthersatisfies HVT61=3.3498 mm; HVT62=3.9860 mm; and HVT61/HVT62=0.8404,where HVT61 a distance perpendicular to the optical axis between thecritical point on the object-side surface 162 of the sixth lens 160 andthe optical axis; and HVT62 a distance perpendicular to the optical axisbetween the critical point on the image-side surface 164 of the sixthlens 160 and the optical axis.

The optical image capturing system 10 of the first embodiment furthersatisfies InRS71=−0.2756 mm; InRS72=−0.0938 mm; and ∥nRS72|/TP7=0.0839,where InRS71 is a displacement in parallel with the optical axis from apoint on the object-side surface 172 of the seventh lens 170, throughwhich the optical axis passes, to a point at the maximum effective semidiameter of the object-side surface 172 of the seventh lens 170; InRS72is a displacement in parallel with the optical axis from a point on theimage-side surface 174 of the seventh lens 170, through which theoptical axis passes, to a point at the maximum effective semi diameterof the image-side surface 174 of the seventh lens 170; and TP7 is acentral thickness of the seventh lens 170 on the optical axis. It ishelpful for manufacturing and shaping of the lenses and is helpful toreduce the size.

The optical image capturing system 10 of the first embodiment satisfiesHVT71=3.6822 mm; HVT72=4.0606 mm; and HVT71/HVT72=0.9068, where HVT71 adistance perpendicular to the optical axis between the critical point onthe object-side surface 172 of the seventh lens 170 and the opticalaxis; and HVT72 a distance perpendicular to the optical axis between thecritical point on the image-side surface 174 of the seventh lens 170 andthe optical axis.

The optical image capturing system 10 of the first embodiment satisfiesHVT72/HOI=0.5414. It is helpful for correction of the aberration of theperipheral view field of the optical image capturing system.

The optical image capturing system 10 of the first embodiment satisfiesHVT72/HOS=0.1505. It is helpful for correction of the aberration of theperipheral view field of the optical image capturing system.

The second lens 120, the third lens 130, and the seventh lens 170 havenegative refractive power. The optical image capturing system 10 of thefirst embodiment further satisfies1≤NA7/NA2, where NA2 is an Abbe numberof the second lens 120; and NA7 is an Abbe number of the seventh lens170. It may correct the aberration of the optical image capturingsystem.

The optical image capturing system 10 of the first embodiment furthersatisfies |TDT|=2.5678%; |ODT|=2.1302%, where TDT is TV distortion; andODT is optical distortion.

For the fifth lens 150 of the optical image capturing system 10 in thefirst embodiment, a transverse aberration at 0.7 field of view in thepositive direction of the tangential fan after the shortest operationwavelength of visible light passing through the edge of the aperture 100is denoted by PSTA, and is 0.00040 mm; a transverse aberration at 0.7field of view in the positive direction of the tangential fan after thelongest operation wavelength of visible light passing through the edgeof the aperture 100 is denoted by PLTA, and is −0.009 mm; a transverseaberration at 0.7 field of view in the negative direction of thetangential fan after the shortest operation wavelength of visible lightpassing through the edge of the aperture 100 is denoted by NSTA, and is−0.002 mm; a transverse aberration at 0.7 field of view in the negativedirection of the tangential fan after the longest operation wavelengthof visible light passing through the edge of the aperture 100 is denotedby NLTA, and is −0.016 mm; a transverse aberration at 0.7 field of viewof the sagittal fan after the shortest operation wavelength of visiblelight passing through the edge of the aperture 100 is denoted by SSTA,and is 0.018 mm; a transverse aberration at 0.7 field of view of thesagittal fan after the longest operation wavelength of visible lightpassing through the edge of the aperture 100 is denoted by SLTA, and is0.016 mm.

The parameters of the lenses of the first embodiment are listed in Table1 and Table 2.

TABLE 1 f = 4.3019 mm; f/HEP = 1.2; HAF = 59.9968 deg Focal Radius ofcurvature Thickness Refractive Abbe length Surface (mm) (mm) Materialindex number (mm) 0 Object plane infinity 1 1^(st) lens −1079.4999642.276 plastic 1.565 58.00 −14.53 2 8.304149657 4.552 3 2^(nd) lens14.39130913 5.240 plastic 1.650 21.40 24.25 4 130.0869482 0.162 5 3^(rd)lens 8.167310118 0.837 plastic 1.650 21.40 −97.07 6 6.944477468 1.450 7Aperture plane 0.477 8 4^(th) lens 121.5965254 2.002 plastic 1.565 58.009.75 9 −5.755749302 1.515 10 5^(th) lens −86.27705938 4.271 plastic1.565 58.00 7.16 11 −3.942936258 0.050 12 6^(th) lens 4.867364751 0.300plastic 1.650 21.40 −6.52 13 2.220604983 0.211 14 7^(th) lens1.892510651 1.118 plastic 1.650 21.40 8.29 15 2.224128115 1.400 16Infrared plane 0.200 BK_7 1.517 64.2 rays filter 17 plane 0.917 18 Imageplane plane Reference wavelength (d-line): 555 nm.

TABLE 2 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k2.500000E+01 −4.711931E−01 1.531617E+00 −1.153034E+01  −2.915013E+00 4.886991E+00 −3.459463E+01 A4 5.236918E−06 −2.117558E−04 7.146736E−054.353586E−04 5.793768E−04 −3.756697E−04  −1.292614E−03 A6 −3.014384E−08 −1.838670E−06 2.334364E−06 1.400287E−05 2.112652E−04 3.901218E−04−1.602381E−05 A8 −2.487400E−10   9.605910E−09 −7.479362E−08 −1.688929E−07  −1.344586E−05  −4.925422E−05  −8.452359E−06 A101.170000E−12 −8.256000E−11 1.701570E−09 3.829807E−08 1.000482E−064.139741E−06  7.243999E−07 A12 0.000000E+00  0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00 A14 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface 9 10 11 12 13 14 15 k −7.549291E+00 −5.000000E+01 −1.740728E+00  −4.709650E+00 −4.509781E+00 −3.427137E+00 −3.215123E+00 A4 −5.583548E−03 1.240671E−04 6.467538E−04 −1.872317E−03 −8.967310E−04−3.189453E−03 −2.815022E−03  A6  1.947110E−04 −4.949077E−05 −4.981838E−05  −1.523141E−05 −2.688331E−05 −1.058126E−05 1.884580E−05 A8−1.486947E−05 2.088854E−06 9.129031E−07 −2.169414E−06 −8.324958E−07 1.760103E−06 −1.017223E−08  A10 −6.501246E−08 −1.438383E−08 7.108550E−09 −2.308304E−08 −6.184250E−09 −4.730294E−08 3.660000E−12 A12 0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00  0.000000E+00 0.000000E+00 0.000000E+00 A14  0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00  0.000000E+00 0.000000E+00

The figures related to the profile curve lengths obtained based on Table1 and Table 2 are listed in the following table:

First embodiment (Reference wavelength: 555 nm) ARE ARE − 1/2 2(ARE/ARE/ ARE 1/2(HEP) value (HEP) HEP) % TP TP (%) 11 1.792 1.792 −0.0004499.98% 2.276 78.73% 12 1.792 1.806 0.01319 100.74% 2.276 79.33% 21 1.7921.797 0.00437 100.24% 5.240 34.29% 22 1.792 1.792 −0.00032 99.98% 5.24034.20% 31 1.792 1.808 0.01525 100.85% 0.837 216.01% 32 1.792 1.8190.02705 101.51% 0.837 217.42% 41 1.792 1.792 −0.00041 99.98% 2.00289.50% 42 1.792 1.825 0.03287 101.83% 2.002 91.16% 51 1.792 1.792−0.00031 99.98% 4.271 41.96% 52 1.792 1.845 0.05305 102.96% 4.271 43.21%61 1.792 1.818 0.02587 101.44% 0.300 606.10% 62 1.792 1.874 0.08157104.55% 0.300 624.67% 71 1.792 1.898 0.10523 105.87% 1.118 169.71% 721.792 1.885 0.09273 105.17% 1.118 168.59% ARS ARS − (ARS/ ARS/ ARS EHDvalue EHD EHD) % TP TP (%) 11 15.095 15.096 0.001 100.01% 2.276 663.24%12 10.315 11.377 1.062 110.29% 2.276 499.86% 21 7.531 8.696 1.166115.48% 5.240 165.96% 22 4.759 4.881 0.122 102.56% 5.240 93.15% 31 3.6324.013 0.382 110.51% 0.837 479.55% 32 2.815 3.159 0.344 112.23% 0.837377.47% 41 2.967 2.971 0.004 100.13% 2.002 148.38% 42 3.402 3.828 0.426112.53% 2.002 191.20% 51 4.519 4.523 0.004 100.10% 4.271 105.91% 525.016 5.722 0.706 114.08% 4.271 133.99% 61 5.019 5.823 0.805 116.04%0.300 1941.14% 62 5.629 6.605 0.976 117.34% 0.300 2201.71% 71 5.6346.503 0.869 115.43% 1.118 581.54% 72 6.488 7.152 0.664 110.24% 1.118639.59%

The detail parameters of the first embodiment are listed in Table 1, inwhich the unit of the radius of curvature, thickness, and focal lengthare millimeter, and surface 0-10 indicates the surfaces of all elementsin the system in sequence from the object side to the image side. Table2 is the list of coefficients of the aspheric surfaces, in which A1-A20indicate the coefficients of aspheric surfaces from the first order tothe twentieth order of each aspheric surface. The following embodimentshave the similar diagrams and tables, which are the same as those of thefirst embodiment, so we do not describe it again.

Second Embodiment

As shown in FIG. 2A and FIG. 2B, an optical image capturing system 20 ofthe second embodiment of the present invention includes, along anoptical axis from an object side to an image side, a first lens 210, asecond lens 220, a third lens 230, an aperture 200, a fourth lens 240, afifth lens 250, a sixth lens 260, a seven lens 270, an infrared raysfilter 280, an image plane 290, and an image sensor 292. FIG. 2C is atransverse aberration diagram at 0.7 field of view of the secondembodiment of the present application.

The first lens 210 has negative refractive power and is made of glass.An object-side surface 212 thereof, which faces the object side, is aconvex surface, and an image-side surface 214 thereof, which faces theimage side, is a concave surface.

The second lens 220 has negative refractive power and is made of glass.An object-side surface 222 thereof, which faces the object side, is aconcave surface, and an image-side surface 224 thereof, which faces theimage side, is a concave surface.

The third lens 230 has positive refractive power and is made of plastic.An object-side surface 232, which faces the object side, is a convexaspheric surface, and an image-side surface 234, which faces the imageside, is a convex aspheric surface.

The fourth lens 240 has positive refractive power and is made ofplastic. An object-side surface 242, which faces the object side, is aconvex aspheric surface, and an image-side surface 244, which faces theimage side, is a convex aspheric surface. The image-side surface 244 hastwo inflection points.

The fifth lens 250 has negative refractive power and is made of plastic.An object-side surface 252, which faces the object side, is a convexaspheric surface, and an image-side surface 254, which faces the imageside, is a concave aspheric surface. The object-side surface 252 has aninflection point.

The sixth lens 260 has positive refractive power and is made of plastic.An object-side surface 262, which faces the object side, is a convexaspheric surface, and an image-side surface 264, which faces the imageside, is a convex aspheric surface. The image-side surface 264 has aninflection point. Whereby, incident angle of each field of view for thesixth lens can be effectively adjusted to improve aberration.

The seventh lens 270 has negative refractive power and is made ofplastic. An object-side surface 272, which faces the object side, is aconvex surface, and an image-side surface 274, which faces the imageside, is a concave surface. It may help to shorten the back focal lengthto keep small in size. In addition, the object-side surface 272 and theimage-side surface 274 both have an inflection point, which may reducean incident angle of the light of an off-axis field of view and correctthe aberration of the off-axis field of view.

The infrared rays filter 280 is made of glass and between the seventhlens 270 and the image plane 290. The infrared rays filter 280 gives nocontribution to the focal length of the system.

The parameters of the lenses of the second embodiment are listed inTable 3 and Table 4.

TABLE 3 f = 2.5840 mm; f/HEP = 1.2; HAF = 100 deg Focal Radius ofcurvature Thickness Refractive Abbe length Surface (mm) (mm) Materialindex number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 98.54233146 8.047glass 1.834 37.16 −18.733 2 13.03803836 8.545 3 2^(nd) lens −63.144718252.816 glass 1.497 81.61 −19.248 4 11.47206375 3.122 5 3^(rd) lens49.99533973 7.110 plastic 1.661 20.40 41.165 6 −57.4026272 15.535 7Aperture 1E+18 0.276 8 4^(th) lens 8.224850411 4.835 plastic 1.565 58.007.874 9 −7.681153484 0.682 10 5^(th) lens 18.6012531 2.423 plastic 1.66120.40 −6.473 11 3.320632709 1.376 12 6^(th) lens 8.650237652 6.075plastic 1.565 58.00 5.784 13 −3.937994762 0.050 14 7^(th) lens7.919737432 1.981 plastic 1.661 20.40 −19.192 15 4.402750994 1.000 16Infrared 1E+18 0.300 BK_7 1.517 64.2 rays filter 17 1E+18 0.293 18 Image1E+18 0.012 plane Reference wavelength (d-line): 555 nm.

TABLE 4 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 −9.793388E−01 2.973766E+01 −1.282558E+00  A4 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 1.600884E−04 7.627411E−05 3.434528E−04 A6 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 −6.759980E−07  −9.003446E−07 4.838355E−06 A8 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00−1.513934E−09  6.883603E−10 −7.241633E−08  A10 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 8.856071E−12 2.075482E−11 2.415549E−09 A120.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A14 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A16 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 Surface 9 10 11 12 13 14 15 k −1.082510E+01  −2.713995E+00−3.089713E+00  −8.674479E+00  −2.994548E+00  −1.384385E+01−7.048734E+00  A4 2.131522E−04 −1.338022E−03 7.116467E−04 8.630247E−04−7.673225E−05  −3.692189E−04 −3.735106E−03  A6 4.028433E−06−5.103150E−06 −4.937205E−05  5.221615E−06 −9.294062E−07  −5.110795E−057.429126E−06 A8 −2.510669E−07  −3.450694E−07 1.099474E−06 −6.434929E−07 2.043935E−07 −8.617002E−07 1.681013E−06 A10 2.063084E−09  1.103283E−09−5.600144E−09  1.153576E−08 9.372014E−10 −4.741607E−08 −4.222700E−08 A12 0.000000E+00  0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A14 0.000000E+00  0.000000E+00 0.000000E+000.000000E+00 0.000000E+00  0.000000E+00 0.000000E+00 A16 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+000.000000E+00

An equation of the aspheric surfaces of the second embodiment is thesame as that of the first embodiment, and the definitions are the sameas well.

The exact parameters of the second embodiment based on Table 3 and Table4 are listed in the following table:

Second embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3||f/f4| |f/f5| |f/f6| 0.1379 0.1342 0.0628 0.3282 0.3992 0.4467 |f/f7|ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 0.1346 0.9723 0.6714 1.4482 3.30700.0193 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 0.9732 0.46765.8916 0.3343 HOS InTL HOS/HOI InS/HOS ODT % TDT % 64.4768  62.8722 12.8954  0.2994 −134.1300   102.4620  HVT11 HVT12 HVT21 HVT22 HVT31HVT32 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 HVT61 HVT62 HVT71 HVT72HVT72/HOI HVT72/HOS 0.0000 0.0000 3.3219 2.9266 0.5853 0.0454 PSTA PLTANSTA NLTA SSTA SLTA 0.010 mm 0.008 mm 0.025 mm −0.013 mm 0.009 mm 0.010mm

The figures related to the profile curve lengths obtained based on Table3 and Table 4 are listed in the following table:

Second embodiment (Reference wavelength: 555 nm) ARE ARE − 1/2 2(ARE/ARE/ ARE 1/2(HEP) value (HEP) HEP) % TP TP (%) 11 1.077 1.076 −0.0006499.94% 8.047 13.37% 12 1.077 1.077 0.00056 100.05% 8.047 13.39% 21 1.0771.076 −0.00061 99.94% 2.816 38.21% 22 1.077 1.078 0.00092 100.09% 2.81638.26% 31 1.077 1.076 −0.00058 99.95% 7.110 15.13% 32 1.077 1.076−0.00060 99.94% 7.110 15.13% 41 1.077 1.079 0.00244 100.23% 4.835 22.32%42 1.077 1.079 0.00246 100.23% 4.835 22.32% 51 1.077 1.077 −0.0001599.99% 2.423 44.43% 52 1.077 1.093 0.01601 101.49% 2.423 45.09% 61 1.0771.079 0.00203 100.19% 6.075 17.76% 62 1.077 1.088 0.01154 101.07% 6.07517.91% 71 1.077 1.079 0.00218 100.20% 1.981 54.47% 72 1.077 1.0840.00730 100.68% 1.981 54.73% ARS ARS − (ARS/ ARS/ ARS EHD value EHD EHD)% TP TP (%) 11 24.497 24.756 0.259 101.06% 8.047 307.65% 12 11.65014.409 2.759 123.68% 8.047 179.07% 21 11.459 11.523 0.064 100.56% 2.816409.16% 22 9.072 10.464 1.391 115.34% 2.816 371.55% 31 9.104 9.291 0.187102.06% 7.110 130.68% 32 8.848 8.902 0.054 100.61% 7.110 125.21% 414.851 5.220 0.368 107.59% 4.835 107.96% 42 4.718 4.796 0.078 101.66%4.835 99.20% 51 4.404 4.428 0.024 100.54% 2.423 182.74% 52 4.497 4.9620.465 110.33% 2.423 204.77% 61 5.152 5.470 0.318 106.18% 6.075 90.04% 625.210 5.701 0.491 109.42% 6.075 93.86% 71 4.733 5.035 0.302 106.37%1.981 254.23% 72 5.324 5.845 0.521 109.79% 1.981 295.14%

The results of the equations of the second embodiment based on Table 3and Table 4 are listed in the following table:

Values related to the inflection points of the second embodiment(Reference wavelength: 555 nm) HIF421 3.3410 HIF421/HOI 0.6682 SGI421−0.5114 |SGI421|/(|SGI421| + TP4) 0.0957 HIF422 4.5580 HIF422/HOI 0.9116SGI422 −0.7798 |SGI422|/(|SGI422| + TP4) 0.1389 HIF511 1.7724 HIF511/HOI0.3545 SGI511 0.0707 |SGI511|/(|SGI511| + TP5) 0.0284 HIF621 4.1717HIF621/HOI 0.8343 SGI621 −1.5864 |SGI621|/(|SGI621| + TP6) 0.2071 HIF7112.0427 HIF711/HOI 0.4085 SGI711 0.2126 |SGI711|/(|SGI711| + TP7) 0.0969HIF721 1.5165 HIF721/HOI 0.3033 SGI721 0.2065 |SGI721|/(|SGI721| + TP7)0.0944

Third Embodiment

As shown in FIG. 3A and FIG. 3B, an optical image capturing system ofthe third embodiment of the present invention includes, along an opticalaxis from an object side to an image side, a first lens 310, a secondlens 320, a third lens 330, an aperture 300, a fourth lens 340, a fifthlens 350, a sixth lens 360, a seventh lens 370, an infrared rays filter380, an image plane 390, and an image sensor 392. FIG. 3C is atransverse aberration diagram at 0.7 field of view of the thirdembodiment of the present application.

The first lens 310 has negative refractive power and is made of glass.An object-side surface 312 thereof, which faces the object side, is aconvex surface, and an image-side surface 314 thereof, which faces theimage side, is a concave surface.

The second lens 320 has negative refractive power and is made of glass.An object-side surface 322 thereof, which faces the object side, is aconcave surface, and an image-side surface 324 thereof, which faces theimage side, is a concave surface.

The third lens 330 has positive refractive power and is made of plastic.An object-side surface 332 thereof, which faces the object side, is aconvex aspheric surface, and an image-side surface 334 thereof, whichfaces the image side, is a convex aspheric surface.

The fourth lens 340 has positive refractive power and is made ofplastic. An object-side surface 342, which faces the object side, is aconvex aspheric surface, and an image-side surface 344, which faces theimage side, is a convex aspheric surface.

The fifth lens 350 has negative refractive power and is made of plastic.An object-side surface 352, which faces the object side, is a concaveaspheric surface, and an image-side surface 354, which faces the imageside, is a concave aspheric surface. The image-side surface 354 has aninflection point.

The sixth lens 360 has positive refractive power and is made of plastic.An object-side surface 362, which faces the object side, is a convexsurface, and an image-side surface 364, which faces the image side, is aconvex surface. The image-side surface 364 has an inflection point. Theimage-side surface 364 has an inflection point. Whereby, incident angleof each field of view for the sixth lens can be effectively adjusted toimprove aberration.

The seventh lens 370 has positive refractive power and is made ofplastic. An object-side surface 372, which faces the object side, is aconvex surface, and an image-side surface 374, which faces the imageside, is a concave surface. It may help to shorten the back focal lengthto keep small in size. In addition, the object-side surface 372 and theimage-side surface 374 both have an inflection point, which may reducean incident angle of the light of an off-axis field of view and correctthe aberration of the off-axis field of view.

The infrared rays filter 380 is made of glass and between the seventhlens 370 and the image plane 390. The infrared rays filter 390 gives nocontribution to the focal length of the system.

The parameters of the lenses of the third embodiment are listed in Table5 and Table 6.

TABLE 5 f = 3.7004 mm; f/HEP = 1.2; HAF = 70.0003 deg Radius ofcurvature Thickness Refractive Abbe Focal length Surface (mm) (mm)Material index number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 33.94582896.763 glass 1.497 81.61 −35.421 2 10.8405598 6.930 3 2^(nd) lens−66.97315291 4.236 glass 1.497 81.61 −10.711 4 5.919261013 8.213 53^(rd) lens 20.24799947 5.315 plastic 1.565 54.50 9.832 6 −6.960408704−1.233 7 Aperture 1E+18 2.239 8 4^(th) lens 12.13055189 3.990 plastic1.565 58.00 11.722 9 −12.94165934 0.104 10 5^(th) lens −35.630202321.161 plastic 1.661 20.40 −6.155 11 4.699316236 0.670 12 6^(th) lens5.545669865 3.709 plastic 1.565 58.00 8.516 13 −28.21381415 1.250 147^(th) lens 9.280768369 1.524 plastic 1.661 20.40 −126.918 157.814031928 1.000 16 Infrared 1E+18 0.300 BK_7 1.517 64.2 rays filter 171E+18 0.220 18 Image 1E+18 0.004 plane Reference wavelength (d-line):555 nm.

TABLE 6 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 −1.621510E+01−3.205843E−01  −3.949323E+00  A4 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 −1.852939E−04 5.921411E−04 2.986636E−04 A6 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 −2.358871E−06 −1.079554E−06 2.117306E−05 A8 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00−7.757225E−09 −2.125122E−07  −3.015400E−07  A10 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00  8.671595E−09 1.070195E−087.441789E−09 A12 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A14 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00  0.000000E+00 0.000000E+00 0.000000E+00 A160.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+000.000000E+00 0.000000E+00 Surface 9 10 11 12 13 14 15 k 3.405073E+004.384252E+01 −3.791675E+00  −4.569282E+00  2.754744E+01 2.200788E+00−5.881090E+00  A4 5.091138E−04 3.717279E−06 9.868087E−04 1.287730E−03−7.359233E−04  −5.075236E−03  −2.194556E−03  A6 −2.656989E−05 −7.027377E−05  −4.854722E−05  4.963414E−05 1.664292E−04 −6.448258E−05 −9.316784E−05  A8 3.838327E−07 2.308340E−07 −2.115132E−06 −2.274142E−06  −2.439957E−06  8.434158E−06 5.831964E−07 A10 1.106316E−084.774476E−08 8.591432E−08 6.341487E−08 2.079774E−07 −5.327453E−07 5.216406E−08 A12 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 A14 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A160.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00

An equation of the aspheric surfaces of the third embodiment is the sameas that of the first embodiment, and the definitions are the same aswell.

The exact parameters of the third embodiment based on Table 5 and Table6 are listed in the following table:

Third embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3||f/f4| |f/f5| |f/f6| 0.1045 0.3455 0.3764 0.3157 0.6012 0.4345 |f/f7|ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 0.0292 1.1557 1.0511 1.0995 1.87270.3379 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 3.3069 1.08943.2323 0.7481 HOS InTL HOS/HOI InS/HOS ODT % TDT % 46.3961  44.8723 9.2792 0.3486 −50.8268  32.4748  HVT11 HVT12 HVT21 HVT22 HVT31 HVT320.0000 0.0000 0.0000 0.0000 0.0000 0.0000 HVT61 HVT62 HVT71 HVT72HVT72/HOI HVT72/HOS 0.0000 2.8708 2.3870 2.8135 0.5627 0.0606 PSTA PLTANSTA NLTA SSTA SLTA −0.001 mm 0.012 mm 0.005 mm −0.007 mm 0.012 mm 0.006mm

The figures related to the profile curve lengths obtained based on Table5 and Table 6 are listed in the following table:

Third embodiment (Reference wavelength: 555 nm) ARE ARE − 1/2 2(ARE/ARE/ ARE 1/2(HEP) value (HEP) HEP) % TP TP (%) 11 1.542 1.542 −0.0003199.98% 6.763 22.79% 12 1.542 1.546 0.00440 100.29% 6.763 22.86% 21 1.5421.541 −0.00070 99.95% 4.236 36.38% 22 1.542 1.559 0.01712 101.11% 4.23636.80% 31 1.542 1.542 0.00051 100.03% 5.315 29.02% 32 1.542 1.5530.01134 100.74% 5.315 29.22% 41 1.542 1.545 0.00338 100.22% 3.990 38.73%42 1.542 1.545 0.00270 100.18% 3.990 38.71% 51 1.542 1.542 −0.0003099.98% 1.161 132.74% 52 1.542 1.565 0.02350 101.52% 1.161 134.78% 611.542 1.560 0.01770 101.15% 3.709 42.05% 62 1.542 1.542 0.00005 100.00%3.709 41.57% 71 1.542 1.545 0.00325 100.21% 1.524 101.36% 72 1.542 1.5480.00624 100.40% 1.524 101.56% ARS ARS − (ARS/ ARS/ ARS EHD value EHDEHD) % TP TP (%) 11 20.150 21.573 1.423 107.06% 6.763 318.98% 12 9.78412.200 2.416 124.70% 6.763 180.39% 21 9.711 9.744 0.034 100.35% 4.236230.02% 22 5.267 6.491 1.224 123.24% 4.236 153.22% 31 4.765 4.786 0.020100.42% 5.315 90.04% 32 4.330 4.554 0.224 105.17% 5.315 85.68% 41 5.2315.600 0.370 107.07% 3.990 140.36% 42 4.953 5.102 0.148 103.00% 3.990127.86% 51 4.722 4.880 0.158 103.34% 1.161 420.15% 52 4.518 4.776 0.258105.71% 1.161 411.24% 61 4.743 5.524 0.782 116.48% 3.709 148.94% 624.111 4.227 0.117 102.84% 3.709 113.98% 71 4.085 4.359 0.274 106.70%1.524 285.95% 72 4.772 5.074 0.301 106.32% 1.524 332.84%

The results of the equations of the third embodiment based on Table 5and Table 6 are listed in the following table:

Values related to the inflection points of the third embodiment(Reference wavelength: 555 nm) HIF521 3.1279 HIF521/HOI 0.6256 SGI5210.8716 |SGI521|/(|SGI521| + TP5) 0.4287 HIF621 2.0372 HIF621/HOI 0.4074SGI621 −0.0778 |SGI621|/(|SGI621| + TP6) 0.0205 HIF711 1.3794 HIF711/HOI0.2759 SGI711 0.0857 |SGI711|/(|SGI711| + TP7) 0.0532 HIF721 1.6728HIF721/HOI 0.3346 SGI721 0.1508 |SGI721|/(|SGI721| + TP7) 0.0900

Fourth Embodiment

As shown in FIG. 4A and FIG. 4B, an optical image capturing system 40 ofthe fourth embodiment of the present invention includes, along anoptical axis from an object side to an image side, a first lens 410, asecond lens 420, a third lens 430, an aperture 400, a fourth lens 440, afifth lens 450, a sixth lens 460, a seventh lens 470, an infrared raysfilter 480, an image plane 490, and an image sensor 492. FIG. 4C is atransverse aberration diagram at 0.7 field of view of the fourthembodiment of the present application.

The first lens 410 has negative refractive power and is made of glass.An object-side surface 412 thereof, which faces the object side, is aconvex surface, and an image-side surface 414 thereof, which faces theimage side, is a concave surface.

The second lens 420 has negative refractive power and is made of glass.An object-side surface 422 thereof, which faces the object side, is aconvex surface, and an image-side surface 424 thereof, which faces theimage side, is a concave surface.

The third lens 430 has positive refractive power and is made of plastic.An object-side surface 432 thereof, which faces the object side, is aconvex aspheric surface, and an image-side surface 434 thereof, whichfaces the image side, is a convex aspheric surface.

The fourth lens 440 has positive refractive power and is made ofplastic. An object-side surface 442, which faces the object side, is aconvex aspheric surface, and an image-side surface 444, which faces theimage side, is a convex aspheric surface.

The fifth lens 450 has negative refractive power and is made of plastic.An object-side surface 452, which faces the object side, is a concaveaspheric surface, and an image-side surface 454, which faces the imageside, is a concave aspheric surface. The image-side surface 454 has aninflection point.

The sixth lens 460 has positive refractive power and is made of plastic.An object-side surface 462, which faces the object side, is a convexaspheric surface, and an image-side surface 464, which faces the imageside, is a concave aspheric surface. The object-side surface 462 has aninflection point. Whereby, incident angle of each field of view for thesixth lens can be effectively adjusted to improve aberration.

The seventh lens 470 has positive refractive power and is made ofplastic. An object-side surface 472, which faces the object side, is aconvex surface, and an image-side surface 474, which faces the imageside, is a concave surface. It may help to shorten the back focal lengthto keep small in size. In addition, the image-side surface 474 has aninflection point, which may reduce an incident angle of the light of anoff-axis field of view and correct the aberration of the off-axis fieldof view.

The infrared rays filter 480 is made of glass and between the seventhlens 470 and the image plane 490. The infrared rays filter 480 gives nocontribution to the focal length of the system.

The parameters of the lenses of the fourth embodiment are listed inTable 7 and Table 8.

TABLE 7 f = 3.3456 mm; f/HEP = 1.4; HAF = 86.8332 deg Focal Radius ofcurvature Thickness Refractive Abbe length Surface (mm) (mm) Materialindex number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 46.54000753 1.542glass 1.497 81.61 −20.046 2 8.130670042 4.052 3 2^(nd) lens 42.66004621.174 glass 1.497 81.61 −11.859 4 5.141353862 4.530 5 3^(rd) lens−16.18068305 7.110 plastic 1.583 30.20 21.476 6 −8.232796061 −0.007 7Aperture 1E+18 1.334 8 4^(th) lens 10.48046817 3.934 plastic 1.565 58.007.828 9 −6.6487022 0.807 10 5^(th) lens −19.37453025 1.268 plastic 1.66120.40 −5.220 11 4.35425175 0.337 12 6^(th) lens 9.015757257 2.638plastic 1.565 58.00 12.651 13 −31.31763855 0.050 14 7^(th) lens6.823404226 3.175 plastic 1.565 54.50 11.412 15 −103.6560564 1.000 16Infrared 1E+18 0.300 BK_7 1.517 64.2 rays filter 17 1E+18 3.212 18 Image1E+18 −0.003 plane Reference wavelength (d-line): 555 nm.

TABLE 8 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 −2.640315E+01 −5.005242E+00  −4.876867E+00  A4 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 −1.340098E−03  −9.149564E−04  6.710561E−04 A6 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 2.940553E−05 3.185717E−058.992586E−07 A8 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00−8.525750E−07  −9.181561E−07  2.733277E−07 A10 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 1.682904E−08 1.707379E−08 −1.482143E−08  A120.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A14 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A16 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 Surface 9 10 11 12 13 14 15 k −1.110891E+01 1.404491E+01−7.093979E+00  −2.633995E+01  1.544760E+01 −1.255719E−01  5.000000E+01A4 −6.687328E−04 −7.323605E−04  4.233795E−04 1.573706E−03 2.359075E−04−1.315572E−04  1.432773E−03 A6  1.651346E−05 1.732376E−06 −6.767011E−06 1.268394E−05 4.645380E−06 9.747473E−06 4.487692E−05 A8 −1.890263E−07−2.454137E−07  7.110177E−07 −1.370408E−06  −3.187194E−07  8.207641E−074.352468E−07 A10 −9.801202E−09 2.942279E−08 −2.290236E−08  7.631760E−09−1.442624E−09  −1.917849E−08  8.983065E−08 A12  0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 A14  0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 A16  0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00

An equation of the aspheric surfaces of the fourth embodiment is thesame as that of the first embodiment, and the definitions are the sameas well.

The exact parameters of the fourth embodiment based on Table 7 and Table8 are listed in the following table:

Fourth embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3||f/f4| |f/f5| |f/f6| 0.1669 0.2821 0.1558 0.4274 0.6409 0.2645 |f/f7|ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 0.2932 1.1408 1.0899 1.0467 1.21120.0149 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 1.6903 0.55224.7672 1.2226 HOS InTL HOS/HOI InS/HOS ODT % TDT % 36.4540  31.9449 7.5163 0.4952 −91.9792  63.5487  HVT11 HVT12 HVT21 HVT22 HVT31 HVT320.0000 0.0000 0.0000 0.0000 0.0000 0.0000 HVT61 HVT62 HVT71 HVT72HVT72/HOI HVT72/HOS 0.0000 0.0000 0.0000 1.2532 0.2584 0.0344 PSTA PLTANSTA NLTA SSTA SLTA 0.010 mm 0.010 mm 0.006 mm −0.005 mm 0.005 mm 0.004mm

The figures related to the profile curve lengths obtained based on Table7 and Table 8 are listed in the following table:

Fourth embodiment (Reference wavelength: 555 nm) ARE ARE − 1/2 2(ARE/ARE/ ARE 1/2(HEP) value (HEP) HEP) % TP TP (%) 11 1.195 1.194 −0.0007399.94% 1.542 77.43% 12 1.195 1.198 0.00348 100.29% 1.542 77.71% 21 1.1951.194 −0.00070 99.94% 1.174 101.76% 22 1.195 1.205 0.01014 100.85% 1.174102.68% 31 1.195 1.195 0.00030 100.02% 7.110 16.81% 32 1.195 1.1980.00332 100.28% 7.110 16.85% 41 1.195 1.197 0.00177 100.15% 3.934 30.42%42 1.195 1.200 0.00469 100.39% 3.934 30.49% 51 1.195 1.195 0.00000100.00% 1.268 94.26% 52 1.195 1.206 0.01105 100.92% 1.268 95.13% 611.195 1.197 0.00222 100.19% 2.638 45.37% 62 1.195 1.194 −0.00058 99.95%2.638 45.27% 71 1.195 1.200 0.00527 100.44% 3.175 37.79% 72 1.195 1.194−0.00085 99.93% 3.175 37.60% ARS ARS − (ARS/ ARS/ ARS EHD value EHD EHD)% TP TP (%) 11 13.665 13.869 0.204 101.49% 1.542 899.38% 12 7.336 9.1451.809 124.66% 1.542 592.99% 21 7.267 7.302 0.035 100.48% 1.174 622.19%22 4.639 5.782 1.143 124.65% 1.174 492.70% 31 4.319 4.418 0.099 102.28%7.110 62.13% 32 3.975 4.119 0.144 103.62% 7.110 57.94% 41 4.861 5.1020.241 104.97% 3.934 129.69% 42 4.899 5.115 0.216 104.41% 3.934 130.03%51 4.515 4.679 0.164 103.63% 1.268 369.16% 52 4.838 5.126 0.288 105.95%1.268 404.40% 61 4.938 5.196 0.259 105.24% 2.638 196.97% 62 5.032 5.0520.020 100.39% 2.638 191.48% 71 5.134 5.927 0.794 115.46% 3.175 186.66%72 4.425 4.800 0.376 108.49% 3.175 151.16%

The results of the equations of the fourth embodiment based on Table 7and Table 8 are listed in the following table:

Values related to the inflection points of the fourth embodiment(Reference wavelength: 555 nm) HIF521 4.5653 HIF521/HOI 0.9413 SGI5211.43479 |SGI521|/(|SGI521| + TP5) 0.5309 HIF611 4.5629 HIF611/HOI 0.9408SGI611 1.18695 |SGI611|/(|SGI611| + TP6) 0.3103 HIF721 0.7351 HIF721/HOI0.1516 SGI721 −0.0022 |SGI721|/(|SGI721| + TP7) 0.0007

Fifth Embodiment

As shown in FIG. 5A and FIG. 5B, an optical image capturing system ofthe fifth embodiment of the present invention includes, along an opticalaxis from an object side to an image side, a first lens 510, a secondlens 520, a third lens 530, an aperture 500, a fourth lens 540, a fifthlens 550, a sixth lens 560, a seventh lens 570, an infrared rays filter580, an image plane 590, and an image sensor 592. FIG. 5C is atransverse aberration diagram at 0.7 field of view of the fifthembodiment of the present application.

The first lens 510 has negative refractive power and is made of glass.An object-side surface 512, which faces the object side, is a convexsurface, and an image-side surface 514, which faces the image side, is aconcave surface.

The second lens 520 has negative refractive power and is made ofplastic. An object-side surface 522 thereof, which faces the objectside, is a concave aspheric surface, and an image-side surface 524thereof, which faces the image side, is a concave aspheric surface.

The third lens 530 has positive refractive power and is made of glass.An object-side surface 532, which faces the object side, is a convexsurface, and an image-side surface 534, which faces the image side, is aconvex surface.

The fourth lens 540 has positive refractive power and is made ofplastic. An object-side surface 542, which faces the object side, is aconvex aspheric surface, and an image-side surface 544, which faces theimage side, is a convex aspheric surface.

The fifth lens 550 has negative refractive power and is made of plastic.An object-side surface 552, which faces the object side, is a convexaspheric surface, and an image-side surface 554, which faces the imageside, is a concave aspheric surface. The object-side surface 552 has aninflection point.

The sixth lens 560 can have positive refractive power and is made ofplastic. An object-side surface 562, which faces the object side, is aconvex aspheric surface, and an image-side surface 564, which faces theimage side, is a concave aspheric surface. Whereby, incident angle ofeach field of view for the sixth lens 560 can be effectively adjusted toimprove aberration.

The seventh lens 570 has positive refractive power and is made ofplastic. An object-side surface 572, which faces the object side, is aconvex aspheric surface, and an image-side surface 574, which faces theimage side, is a concave aspheric surface. It may help to shorten theback focal length to keep small in size. In addition, the object-sidesurface 572 has an inflection point, and the image-side surface 574 hastwo inflection points. It may help to shorten the back focal length tokeep small in size.

The infrared rays filter 580 is made of glass and between the seventhlens 570 and the image plane 590. The infrared rays filter 580 gives nocontribution to the focal length of the system.

The parameters of the lenses of the fifth embodiment are listed in Table9 and Table 10.

TABLE 9 f = 3.3159 mm; f/HEP = 1.4; HAF = 87.3705 deg Focal Radius ofcurvature Thickness Refractive Abbe length Surface (mm) (mm) Materialindex number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 79.29254245 1.990glass 1.639 44.87 −17.709 2 9.844238877 6.296 3 2^(nd) lens −164.72850332.485 plastic 1.565 58.00 −9.138 4 5.376385792 5.734 5 3^(rd) lens23.47040742 7.110 glass 1.648 33.79 16.217 6 −16.90359516 6.481 7Aperture 1E+18 1.169 8 4^(th) lens 8.685880265 4.789 plastic 1.565 58.0011.778 9 −23.09032051 0.050 10 5^(th) lens 15.44890532 1.272 plastic1.661 20.40 −7.922 11 3.806876475 0.166 12 6^(th) lens 5.162390835 4.364plastic 1.565 58.00 10.462 13 27.70469458 1.991 14 7^(th) lens6.965522462 4.028 plastic 1.565 58.00 14.193 15 41.08239212 1.000 16Infrared 1E+18 0.300 BK_7 1.517 64.2 rays filter 17 1E+18 0.771 18 Image1E+18 0.005 plane Reference wavelength (d-line): 555 nm.

TABLE 10 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k0.000000E+00 0.000000E+00 1.281030E+01 −6.469935E−01 0.000000E+000.000000E+00 −8.696638E−01  A4 0.000000E+00 0.000000E+00 1.523645E−05−4.295288E−05 0.000000E+00 0.000000E+00 2.899050E−04 A6 0.000000E+000.000000E+00 −2.352972E−06  −1.056579E−05 0.000000E+00 0.000000E+005.466115E−06 A8 0.000000E+00 0.000000E+00 2.775410E−08  7.161477E−080.000000E+00 0.000000E+00 −1.002115E−07  A10 0.000000E+00 0.000000E+00−1.440192E−10  −8.171101E−10 0.000000E+00 0.000000E+00 4.763860E−09 A120.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A14 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A16 0.000000E+000.000000E+00 0.000000E+00  0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 Surface 9 10 11 12 13 14 15 k 7.740431E+00 −5.000000E+01 −2.827263E+00  −1.446874E+00  −4.256547E+01  −3.515176E+00  4.254684E+01A4 1.881134E−04 −2.122113E−03  −6.220064E−04  −5.007680E−04 −6.188593E−04  1.863859E−04 1.061026E−04 A6 −3.750480E−05  1.258015E−052.393570E−05 3.235235E−06 4.045809E−05 −9.260614E−06  −3.546982E−05  A81.464635E−06 2.174555E−07 −6.219053E−07  1.233229E−06 −9.174470E−08 −2.717066E−07  −1.854888E−07  A10 −1.817766E−08  6.305449E−102.194549E−08 −1.914610E−08  3.374409E−08 7.858183E−09 2.087855E−08 A120.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A14 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A16 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00

An equation of the aspheric surfaces of the fifth embodiment is the sameas that of the first embodiment, and the definitions are the same aswell.

The exact parameters of the fifth embodiment based on Table 9 and Table10 are listed in the following table:

Fifth embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3||f/f4| |f/f5| |f/f6| 0.1872 0.3629 0.2045 0.2815 0.4186 0.3170 |f/f7|ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 0.2336 1.0366 0.9687 1.0701 1.89880.6004 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 1.9380 0.56353.3350 1.3794 HOS InTL HOS/HOI InS/HOS ODT % TDT % 49.9999  47.9238 10.1833  0.3981 −93.1996  67.6830  HVT11 HVT12 HVT21 HVT22 HVT31 HVT320.0000 0.0000 0.0000 0.0000 0.0000 0.0000 HVT61 HVT62 HVT71 HVT72HVT72/HOI HVT72/HOS 0.0000 0.0000 0.0000 3.6891 0.7513 0.0738 PSTA PLTANSTA NLTA SSTA SLTA 0.038 mm −0.001 mm −0.005 mm 0.001 mm 0.007 mm 0.001mm

The figures related to the profile curve lengths obtained based on Table9 and Table 10 are listed in the following table:

Fifth embodiment (Reference wavelength: 555 nm) ARE ARE − 1/2 2(ARE/ARE/ ARE 1/2(HEP) value (HEP) HEP) % TP TP (%) 11 1.184 1.184 −0.00022 99.98% 1.990 59.51% 12 1.184 1.187 0.00261 100.22% 1.990 59.65% 211.184 1.184 −0.00025  99.98% 2.485 47.66% 22 1.184 1.194 0.00932 100.79%2.485 48.04% 31 1.184 1.185 0.00024 100.02% 7.110 16.66% 32 1.184 1.1850.00071 100.06% 7.110 16.67% 41 1.184 1.188 0.00347 100.29% 4.789 24.80%42 1.184 1.185 0.00025 100.02% 4.789 24.74% 51 1.184 1.185 0.00052100.04% 1.272 93.14% 52 1.184 1.201 0.01655 101.40% 1.272 94.40% 611.184 1.194 0.00973 100.82% 4.364 27.36% 62 1.184 1.184 0.00005 100.00%4.364 27.14% 71 1.184 1.189 0.00523 100.44% 4.028 29.53% 72 1.184 1.184−0.00009  99.99% 4.028 29.40% ARS ARS − (ARS/ ARS/ ARS EHD value EHDEHD) % TP TP (%) 11 15.611 15.714 0.102 100.66% 1.990 789.77% 12  8.87811.063 2.185 124.61% 1.990 556.02% 21  8.839  8.889 0.051 100.57% 2.485357.79% 22  6.974  8.495 1.521 121.80% 2.485 341.91% 31  7.514  7.6480.134 101.78% 7.110 107.56% 32  7.457  7.722 0.265 103.56% 7.110 108.60%41  5.376  5.919 0.543 110.11% 4.789 123.61% 42  5.027  5.096 0.070101.38% 4.789 106.43% 51  4.899  4.999 0.101 102.06% 1.272 393.02% 52 4.733  5.166 0.432 109.14% 1.272 406.10% 61  5.021  5.638 0.616 112.28%4.364 129.19% 62  4.657  4.741 0.084 101.81% 4.364 108.64% 71  5.220 5.455 0.234 104.48% 4.028 135.40% 72  5.182  5.190 0.008 100.15% 4.028128.83%

The results of the equations of the fifth embodiment based on Table 9and Table 10 are listed in the following table:

Values related to the inflection points of the fifth embodiment(Reference wavelength: 555 nm) HIF511 1.2943 HIF511/HOI 0.2636 SGI5110.0443 |SGI511|/(|SGI511| + TP5) 0.0337 HIF711 4.0913 HIF711/HOI 0.8333SGI711 1.0132 |SGI711|/(|SGI711| + TP7) 0.2010 HIF721 2.4675 HIF721/HOI0.5026 SGI721 0.0731 |SGI721|/(|SGI721| + TP7) 0.0178 HIF722 4.8965HIF722/HOI 0.9973 SGI722 0.0370 |SGI722|/(|SGI722| + TP7) 0.0091

Sixth Embodiment

As shown in FIG. 6A and FIG. 6B, an optical image capturing system ofthe sixth embodiment of the present invention includes, along an opticalaxis from an object side to an image side, a first lens 610, a secondlens 620, a third lens 630, an aperture 600, a fourth lens 640, a fifthlens 650, a seventh lens 660, a seventh lens 670, an infrared raysfilter 680, an image plane 690, and an image sensor 692. FIG. 6C is atransverse aberration diagram at 0.7 field of view of the sixthembodiment of the present application.

The first lens 610 has negative refractive power and is made of plastic.An object-side surface 612, which faces the object side, is a convexaspheric surface, and an image-side surface 614, which faces the imageside, is a concave aspheric surface.

The second lens 620 has negative refractive power and is made of glass.An object-side surface 622 thereof, which faces the object side, is aconcave surface, and an image-side surface 624 thereof, which faces theimage side, is a concave surface.

The third lens 630 has positive refractive power and is made of glass.An object-side surface 632, which faces the object side, is a convexsurface, and an image-side surface 634, which faces the image side, is aconvex surface.

The fourth lens 640 has positive refractive power and is made ofplastic. An object-side surface 642, which faces the object side, is aconvex aspheric surface, and an image-side surface 644, which faces theimage side, is a convex aspheric surface. The object-side surface 642has an inflection point.

The fifth lens 650 has negative refractive power and is made of plastic.An object-side surface 652, which faces the object side, is a concaveaspheric surface, and an image-side surface 654, which faces the imageside, is a concave aspheric surface.

The sixth lens 660 can have positive refractive power and is made ofplastic. An object-side surface 662, which faces the object side, is aconvex surface, and an image-side surface 664, which faces the imageside, is a convex surface. The image-side surface 664 has an inflectionpoint. Whereby, incident angle of each field of view for the sixth lens660 can be effectively adjusted to improve aberration.

The seventh lens 670 has negative refractive power and is made ofplastic. An object-side surface 672, which faces the object side, is aconvex aspheric surface, and an image-side surface 674, which faces theimage side, is a concave aspheric surface. The object-side surface 672and the image-side surface 674 both have an inflection point. It mayhelp to shorten the back focal length to keep small in size. Inaddition, it may reduce an incident angle of the light of an off-axisfield of view and correct the aberration of the off-axis field of view.

The infrared rays filter 680 is made of glass and between the seventhlens 670 and the image plane 690. The infrared rays filter 680 gives nocontribution to the focal length of the system.

The parameters of the lenses of the sixth embodiment are listed in Table11 and Table 12.

TABLE 11 f = 2.9357 mm; f/HEP = 1.4; HAF = 87.8988 deg Focal Radius ofcurvature Thickness Refractive Abbe length Surface (mm) (mm) Materialindex number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 69.71267258 1.745plastic 1.565 58.00 −19.063 2 9.270067826 5.806 3 2^(nd) lens−51.85977487 3.210 glass 1.497 81.61 −11.657 4 6.673018801 9.752 53^(rd) lens 26.29692654 6.976 glass 1.518 58.96 17.241 6 −12.36279678−0.044 7 Aperture 1E+18 2.199 8 4^(th) lens 10.13972299 5.903 plastic1.565 58.00 9.193 9 −8.460758726 1.188 10 5^(th) lens −21.33414366 1.279plastic 1.661 20.40 −5.192 11 4.231422687 0.821 12 6^(th) lens6.517515126 6.335 plastic 1.565 58.00 5.866 13 −4.400108588 0.426 147^(th) lens 14.32042164 1.720 plastic 1.661 20.40 −34.616 15 8.4128914261.000 16 Infrared 1E+18 0.300 BK_7 1.517 64.2 rays filter 17 1E+18 0.07818 Image 1E+18 −0.010 plane Reference wavelength (d-line): 555 nm.

TABLE 12 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 5.111588E−01 A4 3.433933E−06 −1.452185E−04  0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 −1.345456E−04  A6 5.609725E−09−1.594589E−07  0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00−8.855242E−06  A8 1.541678E−11 6.636487E−09 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 2.397949E−07 A10 −9.804783E−14  −1.254856E−10 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 −1.529222E−08  A120.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A14 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A16 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 Surface 9 10 11 12 13 14 15 k −1.371205E+01 9.665421E+00−5.113418E+00  −8.120128E+00  −3.137365E+00  −3.550208E+01−1.899907E+01  A4 −2.389682E−04 −7.479551E−04  7.749378E−04 1.084045E−03−1.098578E−04  −2.157951E−03 −2.728863E−03  A6 −1.243576E−05−6.626993E−06  −4.001418E−05  −2.069454E−05  2.236554E−05  4.148424E−052.435592E−06 A8 −4.111459E−07 −4.123902E−08  1.461897E−06 1.011778E−07−1.297320E−06  −3.273827E−06 6.742245E−07 A10  9.407077E−09 1.126886E−08−2.185525E−08  5.510130E−09 2.259613E−08 −7.747960E−09 −1.989825E−08 A12  0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A14  0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00  0.000000E+00 0.000000E+00 A16  0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+000.000000E+00

An equation of the aspheric surfaces of the sixth embodiment is the sameas that of the first embodiment, and the definitions are the same aswell.

The exact parameters of the sixth embodiment based on Table 11 and Table12 are listed in the following table:

Sixth embodiment (Reference wavelength: 555nm) |f/f1| |f/f2| |f/f3||f/f4| |f/f5| |f/f6| 0.1540 0.2519 0.1703 0.3193 0.5655 0.5005 |f/f7|ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 0.0848 1.0749 0.9713 1.1067 1.97780.1452 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 1.6354 0.67612.3524 0.3388 HOS InTL HOS/HOI InS/HOS ODT % TDT % 48.6838  47.3160 9.8750 0.4362 −93.8387  76.0219  HVT11 HVT12 HVT21 HVT22 HVT31 HVT320.0000 0.0000 0.0000 0.0000 0.0000 0.0000 HVT61 HVT62 HVT71 HVT72HVT72/HOI HVT72/HOS 0.0000 0.0000 2.4625 2.6031 0.5280 0.0535 PSTA PLTANSTA NLTA SSTA SLTA 0.006 mm 0.003 mm 0.014 mm −0.008 mm 0.008 mm 0.006mm

The figures related to the profile curve lengths obtained based on Table11 and Table 12 are listed in the following table:

Sixth embodiment (Reference wavelength: 555 nm) ARE ARE − 1/2 2(ARE/ARE/ ARE 1/2(HEP) value (HEP) HEP) % TP TP (%) 11 1.048 1.048 −0.00044 99.96% 1.745 60.06% 12 1.048 1.050  0.00175 100.17% 1.745 60.18% 211.048 1.048 −0.00041  99.96% 3.210 32.65% 22 1.048 1.052  0.00388100.37% 3.210 32.78% 31 1.048 1.048 −0.00020  99.98% 6.976 15.03% 321.048 1.049  0.00078 100.07% 6.976 15.04% 41 1.048 1.050  0.00139100.13% 5.903 17.78% 42 1.048 1.050  0.00195 100.19% 5.903 17.79% 511.048 1.048 −0.00001 100.00% 1.279 82.00% 52 1.048 1.057  0.00895100.85% 1.279 82.70% 61 1.048 1.052  0.00374 100.36% 6.335 16.61% 621.048 1.057  0.00871 100.83% 6.335 16.69% 71 1.048 1.049  0.00023100.02% 1.720 60.97% 72 1.048 1.050  0.00156 100.15% 1.720 61.05% ARSARS − (ARS/ ARS/ ARS EHD value EHD EHD) % TP TP (%) 11 14.598 14.7430.145 100.99% 1.745 844.87% 12  8.563 10.251 1.688 119.71% 1.745 587.42%21  8.221  8.256 0.035 100.42% 3.210 257.19% 22  5.376  6.249 0.874116.25% 3.210 194.68% 31  4.778  4.805 0.026 100.55% 6.976  68.88% 32 4.104  4.182 0.079 101.91% 6.976  59.96% 41  4.797  4.936 0.139 102.90%5.903  83.61% 42  5.040  5.277 0.237 104.69% 5.903  89.38% 51  4.488 4.624 0.136 103.03% 1.279 361.62% 52  4.680  5.019 0.339 107.25% 1.279392.52% 61  5.370  5.776 0.406 107.56% 6.335  91.18% 62  5.360  5.8390.479 108.93% 6.335  92.16% 71  4.747  5.156 0.409 108.62% 1.720 299.75%72  5.373  5.877 0.504 109.39% 1.720 341.71%

The results of the equations of the sixth embodiment based on Table 11and Table 12 are listed in the following table:

Values related to the inflection points of the sixth embodiment(Reference wavelength: 555 nm) HIF411 4.1152 HIF411/HOI 0.8347 SGI4110.8116 |SGI411|/(|SGI411| + TP4) 0.1209 HIF621 4.9360 HIF621/HOI 1.0012SGI621 −1.9006 |SGI621|/(|SGI621| + TP6) 0.2308 HIF711 1.3794 HIF711/HOI0.2798 SGI711 0.0543 |SGI711|/(|SGI711| + TP7) 0.0306 HIF721 1.4085HIF721/HOI 0.2857 SGI721 0.0952 |SGI721|/(|SGI721| + TP7) 0.0524

Seventh Embodiment

As shown in FIG. 7A and FIG. 7B, an optical image capturing system ofthe seventh embodiment of the present invention includes, along anoptical axis from an object side to an image side, a first lens 710, asecond lens 720, a third lens 730, an aperture 700, a fourth lens 740, afifth lens 750, a seventh lens 760, a seventh lens 770, an infrared raysfilter 780, an image plane 790, and an image sensor 792. FIG. 7C is atransverse aberration diagram at 0.7 field of view of the seventhembodiment of the present application.

The first lens 710 has negative refractive power and is made of plastic.An object-side surface 712, which faces the object side, is a convexaspheric surface, and an image-side surface 714, which faces the imageside, is a concave aspheric surface.

The second lens 720 has negative refractive power and is made of glass.An object-side surface 722 thereof, which faces the object side, is aconcave surface, and an image-side surface 724 thereof, which faces theimage side, is a concave surface.

The third lens 730 has positive refractive power and is made of plastic.An object-side surface 732, which faces the object side, is a convexaspheric surface, and an image-side surface 734, which faces the imageside, is a convex aspheric surface. The image-side surface 734 has aninflection point.

The fourth lens 740 has positive refractive power and is made of glass.An object-side surface 742, which faces the object side, is a convexsurface, and an image-side surface 744, which faces the image side, is aconvex surface.

The fifth lens 750 has negative refractive power and is made of plastic.An object-side surface 752, which faces the object side, is a concaveaspheric surface, and an image-side surface 754, which faces the imageside, is a concave aspheric surface.

The sixth lens 760 can have positive refractive power and is made ofplastic. An object-side surface 762, which faces the object side, is aconvex aspheric surface, and an image-side surface 764, which faces theimage side, is a convex aspheric surface. Whereby, incident angle ofeach field of view for the sixth lens 760 can be effectively adjusted toimprove aberration.

The seventh lens 770 has positive refractive power and is made ofplastic. An object-side surface 772, which faces the object side, is aconvex aspheric surface, and an image-side surface 774, which faces theimage side, is a concave aspheric surface. It may help to shorten theback focal length to keep small in size. In addition, it may reduce anincident angle of the light of an off-axis field of view and correct theaberration of the off-axis field of view.

The infrared rays filter 780 is made of glass and between the seventhlens 770 and the image plane 790. The infrared rays filter 780 gives nocontribution to the focal length of the system.

The parameters of the lenses of the sixth embodiment are listed in Table13 and Table 14.

TABLE 13 f = 2.5180 mm; f/HEP = 1.4; HAF = 86.1688 deg Focal Radius ofcurvature Thickness Refractive Abbe length Surface (mm) (mm) Materialindex number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 57.46106742 2.933plastic 1.565 58.00 −14.705 2 7.144136312 9.590 3 2^(nd) lens−81.5058405 2.459 glass 1.497 81.61 −15.006 4 8.31193114 4.544 5 3^(rd)lens 49.83082264 7.105 plastic 1.661 20.40 26.817 6 −26.29827455 7.073 7Aperture 1E+18 −0.758 8 4^(th) lens 7.927292779 1.660 glass 1.569 56.0410.018 9 −18.94808747 2.199 10 5^(th) lens −5.084173604 0.717 plastic1.661 20.40 −6.690 11 38.454899 0.509 12 6^(th) lens 9.427076631 2.984plastic 1.565 58.00 9.985 13 −12.53917791 0.050 14 7^(th) lens6.654595892 5.808 plastic 1.565 58.00 13.596 15 33.37864334 1.000 16Infrared 1E+18 0.300 BK_7 1.517 64.2 rays filter 17 1E+18 1.836 18 Image1E+18 −0.010 plane Reference wavelength (d-line): 555 nm.

TABLE 14 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k−2.222275E+00 −6.424766E−01 0.000000E+00 0.000000E+00 −4.973990E+01 8.158745E+00 0.000000E+00 A4 −1.090534E−06 −8.505061E−05 0.000000E+000.000000E+00 −1.602406E−04  −3.075227E−05  0.000000E+00 A6 −3.000016E−09−1.203890E−06 0.000000E+00 0.000000E+00 3.128798E−06 5.527740E−060.000000E+00 A8  4.811053E−12  1.068873E−08 0.000000E+00 0.000000E+00−4.128080E−08  −1.018747E−07  0.000000E+00 A10 −1.919476E−15−8.819398E−11 0.000000E+00 0.000000E+00 8.925120E−10 2.039615E−090.000000E+00 A12  0.000000E+00  0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 A14  0.000000E+00  0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A16 0.000000E+00  0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 Surface 9 10 11 12 13 14 15 k 0.000000E+00−7.513252E+00 3.496845E+01 −2.851481E+01  −3.260594E+00 −2.325107E−014.712648E+01 A4 0.000000E+00 −9.229179E−04 9.286060E−04 −3.662859E−04 −3.185289E−04 −9.173294E−05 1.862068E−03 A6 0.000000E+00  7.708407E−058.410021E−06 1.982948E−05 −9.087385E−06  2.649562E−06 4.399537E−06 A80.000000E+00 −2.597611E−06 1.573835E−06 1.257166E−07  2.867497E−07−8.076566E−09 −8.715171E−07  A10 0.000000E+00 −6.247813E−09−7.163839E−08  −1.053601E−08  −1.264714E−08 −5.504247E−12 7.757432E−08A12 0.000000E+00  0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00 0.000000E+00 0.000000E+00 A14 0.000000E+00  0.000000E+00 0.000000E+000.000000E+00  0.000000E+00  0.000000E+00 0.000000E+00 A16 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00  0.000000E+000.000000E+00

An equation of the aspheric surfaces of the seventh embodiment is thesame as that of the first embodiment, and the definitions are the sameas well.

The exact parameters of the seventh embodiment based on Table 13 andTable 14 are listed in the following table:

Seventh embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3||f/f4| |f/f5| |f/f6| 0.1712 0.1678 0.0939 0.2513 0.3764 0.2522 |f/f7|ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 0.1852 0.7826 0.7154 1.0939 3.80860.0199 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 0.9799 0.55965.0921 1.9632 HOS InTL HOS/HOI InS/HOS ODT % TDT % 50.0000  46.8741 10.3306  0.3259 −87.1264  73.8566  HVT11 HVT12 HVT21 HVT22 HVT31 HVT320.0000 0.0000 0.0000 0.0000 0.0000 0.0000 HVT61 HVT62 HVT71 HVT72HVT72/HOI HVT72/HOS 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 PSTA PLTANSTA NLTA SSTA SLTA 0.015 mm 0.001 mm −0.006 mm 0.001 mm 0.008 mm 0.003mm

The figures related to the profile curve lengths obtained based on Table13 and Table 14 are listed in the following table:

Seventh embodiment (Reference wavelength: 555 nm) ARE ARE − 1/2 2(ARE/ARE/ ARE 1/2(HEP) value (HEP) HEP) % TP TP (%) 11 0.899 0.899 −0.00026 99.97% 2.933  30.65% 12 0.899 0.901  0.00207 100.23% 2.933  30.73% 210.899 0.899 −0.00028  99.97% 2.459  36.55% 22 0.899 0.901  0.00147100.16% 2.459  36.62% 31 0.899 0.899 −0.00025  99.97% 7.105  12.65% 320.899 0.899 −0.00012  99.99% 7.105  12.66% 41 0.899 0.901  0.00164100.18% 1.660  54.26% 42 0.899 0.899  0.00004 100.00% 1.660  54.16% 510.899 0.903  0.00394 100.44% 0.717 125.97% 52 0.899 0.899 −0.00020 99.98% 0.717 125.39% 61 0.899 0.900  0.00087 100.10% 2.984  30.17% 620.899 0.900  0.00048 100.05% 2.984  30.16% 71 0.899 0.902  0.00245100.27% 5.808  15.53% 72 0.899 0.899 −0.00016  99.98% 5.808  15.48% ARSARS − (ARS/ ARS/ ARS EHD value EHD EHD) % TP TP (%) 11 19.467 19.7480.281 101.45% 2.933 673.21% 12 10.498 13.706 3.207 130.55% 2.933 467.22%21  9.496  9.518 0.021 100.22% 2.459 386.99% 22  6.696  7.784 1.088116.25% 2.459 316.49% 31  6.565  6.575 0.010 100.15% 7.105  92.54% 32 5.806  5.844 0.038 100.66% 7.105  82.26% 41  3.471  3.592 0.121 103.49%1.660 216.31% 42  3.521  3.541 0.020 100.56% 1.660 213.23% 51  3.589 3.717 0.129 103.59% 0.717 518.44% 52  3.978  4.041 0.063 101.58% 0.717563.56% 61  4.552  4.597 0.044 100.98% 2.984 154.06% 62  4.967  5.1930.227 104.57% 2.984 174.06% 71  5.754  6.727 0.973 116.91% 5.808 115.84%72  4.407  4.743 0.336 107.62% 5.808  81.67%

The results of the equations of the seventh embodiment based on Table 13and Table 14 are listed in the following table:

Values related to the inflection points of the seventh embodiment(Reference wavelength: 555 nm) HIF321 4.8777 HIF321/HOI 1.0078 SGI321−0.4551 |SGI321|/(|SGI321| + TP3) 0.0602

Eighth Embodiment

As shown in FIG. 8A and FIG. 8B, an optical image capturing system ofthe eighth embodiment of the present invention includes, along anoptical axis from an object side to an image side, a first lens 810, asecond lens 820, a third lens 830, an aperture 800, a fourth lens 840, afifth lens 850, a seventh lens 860, a seventh lens 870, an infrared raysfilter 880, an image plane 890, and an image sensor 892. FIG. 8C is atransverse aberration diagram at 0.7 field of view of the eighthembodiment of the present application.

The first lens 810 has negative refractive power and is made of plastic.An object-side surface 812, which faces the object side, is a convexaspheric surface, and an image-side surface 814, which faces the imageside, is a concave aspheric surface. The object-side surface 812 and theimage-side surface 814 both have an inflection point.

The second lens 820 has negative refractive power and is made ofplastic. An object-side surface 822 thereof, which faces the objectside, is a convex aspheric surface, and an image-side surface 824thereof, which faces the image side, is a concave aspheric surface. Theobject-side surface 822 and the image-side surface 824 both have aninflection point.

The third lens 830 has positive refractive power and is made of plastic.An object-side surface 832, which faces the object side, is a convexaspheric surface, and an image-side surface 834, which faces the imageside, is a convex aspheric surface. The object-side surface 832 and theimage-side surface 834 both have an inflection point.

The fourth lens 840 has positive refractive power and is made ofplastic. An object-side surface 842, which faces the object side, is aconvex aspheric surface, and an image-side surface 844, which faces theimage side, is a convex aspheric surface.

The fifth lens 850 has negative refractive power and is made of plastic.An object-side surface 852, which faces the object side, is a concaveaspheric surface, and an image-side surface 854, which faces the imageside, is a concave aspheric surface.

The sixth lens 860 can have positive refractive power and is made ofplastic. An object-side surface 862, which faces the object side, is aconcave surface, and an image-side surface 864, which faces the imageside, is a convex surface. The object-side surface 862 and theimage-side surface 864 both have an inflection point. Whereby, incidentangle of each field of view for the sixth lens 860 can be effectivelyadjusted to improve aberration.

The seventh lens 870 has positive refractive power and is made ofplastic. An object-side surface 872, which faces the object side, is aconvex surface, and an image-side surface 874, which faces the imageside, is a concave surface. The image-side surface 874 has an inflectionpoint. It may help to shorten the back focal length to keep small insize. In addition, it may reduce an incident angle of the light of anoff-axis field of view and correct the aberration of the off-axis fieldof view.

The infrared rays filter 880 is made of glass and between the seventhlens 870 and the image plane 890. The infrared rays filter 880 gives nocontribution to the focal length of the system.

In the eighth embodiment, the optical image capturing system of theseventh embodiment further satisfies ΣPP=76.7754 mm; and f3/ΣPP=0.2346,where ΣPP is a sum of the focal lengths of each positive lens. It ishelpful to share the positive refractive power of one single lens toother positive lenses to avoid the significant aberration caused by theincident rays.

The optical image capturing system of the eighth embodiment furthersatisfies ΣNP=−29.9308 mm; and f1/ΣNP=0.4139, where ΣNP is a sum of thefocal lengths of each negative lens. It is helpful to share the negativerefractive power of one single lens to the other negative lenses toavoid the significant aberration caused by the incident rays.

The parameters of the lenses of the sixth embodiment are listed in Table15 and Table 16.

TABLE 15 f = 3.2022 mm; f/HEP = 2.8; HAF = 70 deg Focal Radius ofcurvature Thickness Refractive Abbe length Surface (mm) (mm) Materialindex number (mm) 0 Object plane plane 1 1^(st) lens 45.25194153 1.179plastic 1.565 58.00 −13.615 2 6.530553663 2.979 3 2^(nd) lens28.45048651 0.890 plastic 1.565 58.00 −12.389 4 5.567945123 2.258 53^(rd) lens 16.86317406 13.161 plastic 1.550 56.50 18.014 6 −17.490571420.000 7 Aperture plane 0.050 8 4^(th) lens 3.821831971 2.811 plastic1.565 58.00 4.229 9 −4.7192252 0.686 10 5^(th) lens −3.886344092 0.300plastic 1.650 21.40 −3.927 11 7.853851213 0.493 12 6^(th) lens−16.45040823 0.331 plastic 1.607 26.60 35.403 13 −9.416243867 0.050 147^(th) lens 10.04814497 0.521 plastic 1.565 58.00 19.129 15 134.6580461.000 16 Infrared plane 0.300 BK_7 1.517 64.2 rays filter 17 plane 2.99118 Image plane 0.000 plane Reference wavelength (d-line): 555 nm.

TABLE 16 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k4.758702E+00 −5.889217E−02 −6.943469E+00 −5.931587E−02 −1.196153E+01−2.846770E+01  −6.483847E−02 A4 6.227544E−06 −4.117326E−04 −2.236683E−06 7.492048E−05 −2.173923E−04 8.200135E−04 −2.077686E−04 A6 3.084494E−08−3.728783E−06 −2.602700E−08 −3.594973E−06 −1.336542E−06 2.531078E−04 1.819755E−05 A8 2.405824E−10 −1.816585E−08 −1.089998E−09 −2.096298E−07−6.065276E−09 −1.249497E−06  −1.055843E−05 A10 1.681390E−12 7.136442E−11  2.869754E−12 −1.256432E−08 −1.755005E−09 5.139796E−06−5.651390E−06 A12 5.933250E−15  1.326333E−12 −4.974101E−12 −6.643498E−10 1.305674E−10 4.327953E−20 −3.032302E−16 A14 −7.538093E−17 −2.740915E−13 −8.537290E−14 −7.544791E−12 −2.655221E−12 8.231837E−25−7.192269E−24 A16 0.000000E+00  0.000000E+00  0.000000E+00  0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00 Surface 9 10 11 12 13 14 15 k−1.615455E−01 −1.254414E+00 3.463610E+00 2.303942E+01 −1.893896E+01 −2.877868E+00  5.000000E+01 A4 −5.897570E−04  2.278000E−04 5.564271E−04−4.933293E−04  1.732535E−03 −1.952076E−04  5.340317E−04 A6 −1.825644E−04−6.332738E−04 2.397167E−04 1.095835E−04 1.847862E−04 5.075190E−069.227855E−05 A8  2.019382E−07 −1.577314E−04 −8.070753E−06  8.942415E−051.970939E−05 6.130407E−06 1.629776E−05 A10 −5.333494E−06  6.144598E−077.661629E−06 1.242952E−05 5.071654E−06 4.969750E−07 −7.504117E−07  A12−2.606537E−17 −3.647167E−16 −1.006614E−16  −4.105671E−09  2.954683E−097.578220E−09 3.011747E−09 A14  8.064118E−25 −2.699251E−24 2.566758E−22−5.014763E−22  1.332088E−18 7.114791E−12 −5.940679E−12  A16 0.000000E+00  0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00

An equation of the aspheric surfaces of the eighth embodiment is thesame as that of the first embodiment, and the definitions are the sameas well.

The exact parameters of the eighth embodiment based on Table 15 andTable 16 are listed in the following table:

Eighth embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3||f/f4| |f/f5| |f/f6| 0.2352 0.2585 0.1778 0.7572 0.8155 0.0905 |f/f7|ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 0.1674 1.1928 1.3092 0.9111 0.93020.0156 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 1.0990 0.68774.6700 1.7262 HOS InTL HOS/HOI InS/HOS ODT % TDT % 30.0000  25.7092 6.0000 0.3178 −43.1697  27.8256  HVT11 HVT12 HVT21 HVT22 HVT31 HVT320.0000 0.0000 0.0000 0.0000 0.0000 0.0000 HVT61 HVT62 HVT71 HVT72HVT72/HOI HVT72/HOS 1.9821 2.0599 0.0000 0.0000 0.0000 0.0000 PSTA PLTANSTA NLTA SSTA SLTA 0.003 mm 0.008 mm 0.002 mm −0.002 mm 0.001 mm 0.002mm

The figures related to the profile curve lengths obtained based on Table15 and Table 16 are listed in the following table:

Eighth embodiment (Reference wavelength: 555 nm) ARE ARE − 1/2 2(ARE/ARE/ ARE 1/2(HEP) value (HEP) HEP) % TP TP (%) 11 0.572 0.571 −0.00081 99.86%  1.179  48.45% 12 0.572 0.572 −0.00010  99.98%  1.179  48.51% 210.572 0.571 −0.00079  99.86%  0.890  64.15% 22 0.572 0.572  0.00018100.03%  0.890  64.26% 31 0.572 0.571 −0.00072  99.87% 13.161  4.34% 320.572 0.571 −0.00073  99.87% 13.161  4.34% 41 0.572 0.573  0.00131100.23%  2.811  20.39% 42 0.572 0.572  0.00058 100.10%  2.811  20.36% 510.572 0.573  0.00121 100.21%  0.300 191.01% 52 0.572 0.572 −0.00031 99.95%  0.300 190.50% 61 0.572 0.571 −0.00071  99.88%  0.331 172.62% 620.572 0.571 −0.00050  99.91%  0.331 172.69% 71 0.572 0.571 −0.00052 99.91%  0.521 109.63% 72 0.572 0.571 −0.00083  99.86%  0.521 109.58%ARS ARS − (ARS/ ARS/ ARS EHD value EHD EHD) % TP TP (%) 11 10.175 10.3110.137 101.34%  1.179 874.87% 12  6.299  7.531 1.232 119.55%  1.179639.00% 21  6.256  6.292 0.036 100.58%  0.890 706.81% 22  4.813  5.5510.738 115.33%  0.890 623.56% 31  4.719  4.741 0.023 100.48% 13.161 36.03% 32  1.569  1.570 0.001 100.08% 13.161  11.93% 41  1.830  1.9040.075 104.08%  2.811  67.74% 42  1.990  2.061 0.071 103.59%  2.811 73.33% 51  1.872  1.960 0.087 104.67%  0.300 653.23% 52  2.041  2.0770.036 101.78%  0.300 692.35% 61  2.095  2.098 0.003 100.14%  0.331634.24% 62  2.204  2.208 0.005 100.20%  0.331 667.46% 71  2.583  2.6110.028 101.10%  0.521 501.09% 72  2.658  2.664 0.006 100.22%  0.521511.22%

The results of the equations of the seventh embodiment based on Table 15and Table 16 are listed in the following table:

Values related to the inflection points of the eighth embodiment(Reference wavelength: 555 nm) HIF211 5.4022 HIF211/HOI 1.0804 SGI2110.4801 |SGI211|/(|SGI211| + TP2) 0.3504 HIF221 4.5661 HIF221/HOI 0.9132SGI221 2.1748 |SGI221|/(|SGI221| + TP2) 0.7096 HIF311 3.3316 HIF311/HOI0.6663 SGI311 0.2711 |SGI311|/(|SGI311| + TP3) 0.0202 HIF321 1.3338HIF321/HOI 0.2668 SGI321 −0.0449 |SGI321|/|SGI321| + TP3) 0.0034 HIF6111.4885 HIF611/HOI 0.2977 SGI611 −0.0694 |SGI611|/(|SGI611| + TP6) 0.1735HIF621 1.3418 HIF621/HOI 0.2684 SGI621 −0.0812 |SGI621|/(|SGI621| + TP6)0.1971

It must be pointed out that the embodiments described above are onlysome embodiments of the present invention. All equivalent structureswhich employ the concepts disclosed in this specification and theappended claims should fall within the scope of the present invention.

What is claimed is:
 1. An optical image capturing system, in order along an optical axis from an object side to an image side, comprising: a first lens having negative refractive power; a second lens having refractive power; a third lens having refractive power; a fourth lens having refractive power; a fifth lens having refractive power; a sixth lens having refractive power; a seventh lens having refractive power; and an image plane; wherein the optical image capturing system has a total of the seven lenses with refractive power; the first lens is made of glass; at least five lenses among the second lens to the seventh lens is made of plastic; at least one lens among the second lens to the seventh lens has positive refractive power; each lens among the first lens to the seventh lens has an object-side surface, which faces the object side, and an image-side surface, which faces the image side; wherein the optical image capturing system satisfies: 1.0≤f/HEP≤10.0; 1.2≤IN12/f≤5.0; 0 deg<HAF≤150 deg; and 0.9≤2(ARE/HEP)≤1.5; where f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HAF is a half of a maximum field angle of the optical image capturing system; for any surface of any lens, ARE is a profile curve length measured from a start point where the optical axis passes therethrough, along a surface profile thereof, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis; IN12 is a distance on the optical axis between the first lens and the second lens; wherein the optical image capturing system further satisfies: 0<IN67/f≤0.8; where IN67 is a distance on the optical axis between the sixth lens and the seventh lens.
 2. The optical image capturing system of claim 1, wherein each two neighboring lenses among the first to the seventh lenses are separated by air.
 3. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: 0.9≤ARS/EHD≤2.0; where, for any surface of any lens, EHD is a maximum effective half diameter thereof, ARS is a profile curve length measured from a start point where the optical axis passes therethrough, along a surface profile thereof, and finally to an end point of the maximum effective half diameter thereof.
 4. The optical image capturing system of claim 1, wherein the image plane is either flat or curved.
 5. The optical image capturing system of claim 1, wherein at least one lens among the first lens, the second lens, the third lens, the fourth lens, the fifth lens, the sixth lens, and the seventh lens is configured to filter out light of wavelengths shorter than 500 nm.
 6. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: 0.1≤(TP7+IN67)/TP6≤10; where IN67 is a distance on the optical axis between the sixth lens and the seventh lens; TP6 is a thickness of the sixth lens on the optical axis; TP7 is a thickness of the seventh lens on the optical axis.
 7. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: 0.1≤(TP1+IN12)/TP2≤10; where IN12 is a distance on the optical axis between the first lens and the second lens; TP1 is a thickness of the first lens on the optical axis; TP2 is a thickness of the second lens on the optical axis.
 8. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: 0<TP4/(IN34+TP4+IN45)<1; where IN34 is a distance on the optical axis between the third lens and the fourth lens; IN45 is a distance on the optical axis between the fourth lens and the fifth lens; TP4 is a thickness of the fourth lens on the optical axis. 